Edge-lit waveguide illumination systems employing planar arrays of linear cylindrical lenses

ABSTRACT

An apparatus for distributing light from a planar waveguide through an array of linear cylindrical lenses formed in a major surface of the waveguide, and a method of making the same. Light received on an edge of the waveguide is propagated transmissively and retained by total internal reflection, except in response to impinging upon light deflecting elements which sufficiently redirect the light to escape the waveguide such that the extracted from the waveguide is further redirected and redistributed through the array of linear cylindrical lenses.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation of application Ser. No. 15/838,061filed on Dec. 11, 2017, which is a continuation of application Ser. No.14/969,898 filed on Dec. 15, 2015, which is a continuation ofapplication Ser. No. 12/764,867 filed on Apr. 21, 2010, now U.S. Pat.No. 9,256,007, which claims priority from U.S. provisional applicationSer. No. 61/214,331 filed on Apr. 21, 2009, the disclosure of which isincorporated herein by reference in its entirety, and from U.S.provisional application Ser. No. 61/339,512 filed on Mar. 6, 2010, thedisclosure of which is incorporated herein by reference in its entirety.

STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT

Not Applicable

INCORPORATION-BY-REFERENCE OF MATERIAL SUBMITTED ON A COMPACT DISC

Not Applicable

NOTICE OF MATERIAL SUBJECT TO COPYRIGHT PROTECTION

A portion of the material in this patent document is subject tocopyright protection under the copyright laws of the United States andof other countries. The owner of the copyright rights has no objectionto the facsimile reproduction by anyone of the patent document or thepatent disclosure, as it appears in the United States Patent andTrademark Office publicly available file or records, but otherwisereserves all copyright rights whatsoever. The copyright owner does nothereby waive any of its rights to have this patent document maintainedin secrecy, including without limitation its rights pursuant to 37C.F.R. § 1.14.

BACKGROUND OF THE INVENTION 1. Field of the Invention

The present invention relates to a optical reflecting devices and moreparticularly to an apparatus for collecting or distributing radiantenergy, into or from an optical waveguide.

2. Description of Background Art

Devices for collecting or concentrating a parallel beam ofelectromagnetic energy have conventionally employed reflective mirrorsor refractive lenses. These devices collect energy in a broad spectrumfrom the entire area of the device and focus it onto a smaller areadisposed at a considerable distance above or beneath the device andrequires a fairly complex structure which occupies substantial volume.

Increasingly, light collection systems, including light detectors andconcentrators, need to be configured for inputting light into awaveguide, such as an optical fiber or transparent rectangular plate, soit can be propagated along the waveguide by means of total internalreflection. In a conventional system, the spatially distributed lightflux is input into a waveguide through one of its terminal ends usingrelatively large optical elements such as lenses and mirrors. Althoughthe light guides themselves are typically slim and space efficient, theadditional optics necessary for collecting or distributing the lightover a large area leads to increased cost and system volume. In responseto these shortcomings, the utility of the devices is hampered whilenumerous spatially-sensitive applications are rendered impractical.

Luminescent concentrators are also found in the industry for trappingincident radiation in a light guide by absorbing and re-radiating it inthe form of scattered light at a longer wavelength using luminescentcenters distributed in the volume of the light guide. However, becauseof the scattered nature of the reradiated light, only a portion of itcan become trapped in the light guide by the total internal reflection,while the rest of the light escapes from the light guide. Furthermore,the luminescent centers can absorb or scatter already trapped light thusmaking the light guide less transparent and less efficient.

A holographic concentrator known in the art, utilizes a hologram layerthat bends the incident light by means of diffraction so that it becomestrapped in a transparent light guide. However, at least a portion of thediffracted light is lost at each bounce from the same holographic layerguide due to re-coupling.

None of the previous efforts provides an efficient solution for lightcollection or concentration into a waveguide through its longitudinalface while maintaining a low system profile.

Conventional reflective mirror and refractive lens devices collimateelectromagnetic energy across a broad energy spectrum from the entirearea of the device and either focus it onto a smaller area disposed at aconsiderable distance above or beneath the device or collimate anddirect it into a predetermined direction or onto a target. These devicesare fairly bulky structures occupying substantial volume.

For example, in a conventional system, the primary optical element(e.g., mirror or lens) is focused at the location where the lightemitting or light receiving element is disposed. Considering that thefocus is usually located at a considerable distance from the primaryoptical element, the resulting volume formed by a three-dimensionalshape enveloping the optical element's aperture and the focal point isconsiderably larger than the volume of the optical element itself. Thisincreases system size, weight, and cost, while hampering utility of thesystem.

Many applications require the optical system to provide homogeneousirradiance distribution or another desired illumination pattern on atarget. Examples are projection display systems requiring uniform lightdistribution from a light source on a target screen or optical collectorwhere the light has to be collected and more evenly distributed across alight receiving device.

Numerous light processing systems require light to be input into awaveguide, propagated along the waveguide, and extracted from thewaveguide to illuminate a designated target or pattern. In aconventional system, the light is extracted from a waveguide through oneof its terminal ends and is further collimated by an optical systemwhose focus is disposed in the vicinity of the area where the lightexits the waveguide. The inclusion of additional optics increases costand system volume rendering the designs impractical in space-limitedapplications.

In another conventional system a planar waveguide is employed whichextracts light from a lateral face of the waveguide by means of a numberof light deflecting elements embedded into the waveguide or attached toits lateral face. Although this latter approach is more space efficientthan the former one, the light comes out of the waveguide substantiallyuncollimated due to the inherent divergence of the light propagating inthe waveguide which results in the substantial divergence of lightextracted from the waveguide.

In addition, modern illumination systems often utilize compact anddiscrete light sources, such as Light Emitting Diodes (LEDs). Use ofthese light sources often results in unwanted glare problems,particularly in some general lighting applications or display lights.Typically, these problems are addressed by adding conventional and bulkyoptical systems, collimators and diffusers that at least partiallynegate the advantages of LEDs such as compactness and energy efficiency.

Accordingly, prior illumination efforts have failed to provide anefficient solution for extracting light from a waveguide through itslongitudinal face with efficient light collimation. These needs andothers are met within the present invention, which provides an improvedoptical system for distributing light along a waveguide and extractingthe distributed light from the waveguide with minimum space consumptionand improved light collimation.

BRIEF SUMMARY OF THE INVENTION

The present invention solves a number of light collection anddistribution problems within a compact system. Light is directed througha waveguide configured with deflection means for redirecting lightto/from a collimating means.

In a first portion of the invention, apparatus and methods are describedfor collecting and concentrating radiant energy, more particularly, tocollecting light from a distant light source and injecting the lightinto an optical light guide (also referenced heretofore as a“waveguide”), concentrating light guides, radiation detectors, opticalcouplers, solar thermal and photovoltaic concentrators, and day lightingsystems. In at least one embodiment, the present invention describes acollector which provides light collection in response to collectingincident light by a collector array and injecting the light into aplanar waveguide through its light conducting wall, trapping the lightin the waveguide by means of at least a total internal reflection andguiding the light to a terminal end of the waveguide.

A compact light collection system including a planar waveguide and acollector array are described. The waveguide comprises a plurality oflight deflecting elements optically coupled to the waveguide. Thecollector array comprises a plurality of mini-collectors configured tocollect light from a larger area and focus the incident light ontorespective light deflecting elements characterized by a substantiallysmaller area. Each light deflecting element is configured to receive alight beam and redirect it at an angle with respect to a surface normalangle (perpendicular to both axis) of the prevailing plane of thewaveguide greater than a critical angle at which the light beam becomestrapped in the waveguide and can propagate toward the terminal end ofthe waveguide by optical transmission and total internal reflection(TIR).

Disposed in the radiant energy flux transformation system is a primarylinear focus concentrating collector formed by a plurality ofcylindrical slat-like reflectors and a secondary elongated collector.The reflectors of the primary collector generally have concave or planartransversal profiles and are positioned in a stepped arrangement withlongitudinal axes being parallel to each other and to the secondarycollector. The reflectors are tilted away from the direction of thesource of radiant energy at a range of angles being less than 45° toreflect and direct the incident energy flux to a common focal regionlocated below the primary collector where the concentrated flux isintercepted and further transformed by the secondary collector. Inaddition to efficient concentrating of radiant energy such as sunlight,the system can provide uniformity or a desired energy distribution inthe concentrated flux.

A second portion of the invention describes a device and method forcollimating and distributing radiant energy, more particularly, toguiding the light by an optical waveguide (light guide) and extractingthe light from the waveguide with improved light collimation. Moregenerally, it also relates to a device intercepting the divergent lightfrom a light source and directing the light into a collimated beam suchas flashlights, spotlights, flood lights, LED collimators, lanterns,headlamps, backlight or projection display systems, accent lights,various other illumination devices, optical couplers and switches, andthe like. In at least one embodiment, the present invention describes anilluminator which provides light collimation by extracting light from aplanar waveguide through its lateral light conducting face in responseto an array of discrete light deflecting means optically coupled to thewaveguide and further collimated by a matching array of lightcollimating means. Other objects and advantages of this invention willbe apparent to those skilled in the art from the following disclosure.

The invention is amenable to being embodied in a number of ways,including but not limited to the following descriptions.

At least one embodiment of the invention is configured as an apparatusfor light collimation and distribution, comprising: (a) a planarwaveguide having an optically transparent planar material having edgesdisposed between a first planar surface and a second planar surface; inwhich the planar waveguide is configured to receive light on one edge ofthe planar material, and to propagate the received light through theplanar waveguide in response to optical transmission and total internalreflection; (b) a plurality of light collimating elements within acollimating array which is disposed in an optical receiving relationshipwith a planar surface of the planar waveguide; and (c) a plurality oflight deflecting elements optically coupled to the waveguide andconfigured for deflecting light propagating through the planar waveguideat a sufficiently low angle, below the predetermined critical angle fortotal internal reflection (TIR), with respect to a surface normaldirection of an exterior surface of the planar waveguide to exit theplanar waveguide and enter the collimating array. Each of the pluralityof light deflecting elements is in a predetermined alignment with eachof the plurality of light collimating elements. The device operates inresponse to light received on the edge of the planar waveguide beingangularly redirected, collimated, and distributed from the surface ofthe collimating array which is optically coupled to the planarwaveguide.

In at least one implementation, the plurality of light collimatingelements comprises a parallel array of elongated lenticular lenses, orparallel array of elongated focus mirrors. In at least oneimplementation, the plurality of deflecting elements comprises aparallel array of grooves. These elements and grooves are preferablyelongated, such as in response to comprising a one-dimensional arrayspanning across a width equivalent to the entire waveguide surface, or asubstantial portion thereof. In at least one implementation, the groovesare configured at a slope angle θ₃₀ which is bounded by the relation

${\arcsin \left( \frac{n_{2}}{n_{1}} \right)} \leq \theta_{30} \leq {\arccos \left( \frac{n_{2}}{n_{1}} \right)}$

in which n₁ is the refractive index of the planar waveguide and n₂ isthe refractive index of an outside medium.

In alternative implementations, the grooves can be configured indifferent ways. In at least one implementation, the plurality of lightdeflecting elements comprises grooves within (e.g., cut or molded into)the planar waveguide configured for redirecting the received light inresponse to reflection from at least one surface of the groove towardthe collimating array. In at least one implementation, the lightdeflecting elements comprise grooves formed within each of a pluralityof blocks that are attached and in optical communication with the planarwaveguide, and the grooves are configured for redirecting the receivedlight in response to reflection from at least one surface of the groovetoward the collimating array. In at least one implementation, each ofthe grooves has a transparent surface and a reflective surface, andlight received from the planar waveguide passes through the transparentsurface of each of the grooves to be reflected from the reflectivesurface of each of the grooves toward the collimating array. In at leastone implementation, the grooves comprise a prismatic groove or ridgeformed in a surface of the planar waveguide disposed toward thecollimating array for refractively deflecting the received lightimpinging on the prismatic groove to pass through the prismatic grooveor ridge to exit the planar waveguide.

In at least one implementation, the plurality of light collimatingelements is selected from the group consisting of imaging lenses,non-imaging lenses, spherical lenses, aspherical lenses, lens arrays,Fresnel lenses, TIR lenses, gradient index lenses, diffraction lenses,mirrors, Fresnel mirrors, spherical mirrors, parabolic mirrors, mirrorarrays, and trough mirrors.

In at least one implementation, the plurality of light deflectingelements is selected from the group consisting of planar mirrors, curvedmirrors, prisms, prism arrays, prismatic grooves, surface relieffeatures, reflective surfaces, refractive surfaces, diffractiongratings, holograms, and light scattering elements.

In at least one implementation, an optical interface layer is disposedbetween the planar waveguide and the collimating array. In at least oneimplementation, the optical interface layer has a lower refractive indexthan the planar waveguide, and in at least one implementation, theoptical interface layer comprises air. In at least one implementation,the optical interface layer is selected from the group of opticalmaterials consisting of low refractive index monomers, polymers,fluoropolymers, low-n optical adhesives, thin films, and opticalwaveguide cladding materials.

In at least one implementation, at least one illumination source isoptically coupled to at least one edge of the planar waveguide. In atleast one implementation, one or more illumination sources is opticallycoupled to the edges of one or more cutouts within the planar waveguide.

In at least one implementation, both the collimating array and theplanar waveguide have a round or sectorial shape, such as obtainable inresponse to revolving a cross section of the collimating array and theplanar waveguide around an axis.

In at least one implementation, the collimator array comprises pointfocus lenses, or mirrors, having a shape selected from the groupconsisting of round, rectangular, square, and hexagonal.

In at least one implementation, the planar waveguide comprises arectangular plate having a first terminal edge, a second terminal edge,a first side wall, a second side wall, the first planar surface and thesecond planar surface. Although it should be appreciated that therectangular plate can be bent, or otherwise slightly curved, whileretaining a substantially rectangular planform. And more particularly,the combination of collimator and waveguide, along with any intermediarylayers, are adapted in at least one implementation to support bentand/or rolled configurations. In at least one implementation, a mirroredsurface is added to one or more of the first terminal edge, the secondterminal edge, the first side wall and the second side wall. In at leastone implementation, a cladding layer is added to one or more of thefirst terminal edge, the second terminal edge, the first side wall andthe second side wall.

In at least one implementation, the planar waveguide and collimatorarray are adapted for being retained in a translated, a reversed and/ora rotated orientation relative to each other toward achieving aadjusting the light distribution or collimation pattern. In at least oneimplementation, the planar waveguide and collimator array are adaptedfor being retained in a movable relationship with one another towardadjusting the light distribution or collimation pattern. In at least oneimplementation, a coating is disposed on the exterior of said planarwaveguide and/or said collimator array, such as including any of thefollowing coatings or combination of coatings thereof: anti-reflective,protective, encapsulates, reflective, diffusive, radiation protective,scratch and stain resistant, and light filtering.

At least one embodiment of the invention is configured as an apparatusfor light collimation and distribution, comprising: (a) a planarwaveguide having an optically transparent planar material configured toreceive light on one edge of the planar material, and to propagate thereceived light through the planar waveguide in response to opticaltransmission and total internal reflection; (b) a parallel collimatingarray having a plurality of elongated light collimating lenses disposedin an optical receiving relationship with a planar surface of the planarwaveguide; and (c) a parallel deflecting array having a plurality ofelongated light deflecting grooves within the planar waveguide which areconfigured for deflecting light propagating through the waveguide at asufficiently low angle, below the predetermined critical angle for totalinternal reflection (TIR), with respect to a surface normal direction ofan exterior surface of the planar waveguide to exit the planar waveguideand enter the parallel collimating array. Each of elongated lightdeflecting grooves is preferably positioned in a predetermined alignmentwith each of the plurality of elongated light collimating lenses. Inoperation, the light received on the edge of the planar waveguide isangularly redirected, collimated, and distributed from the surface ofthe parallel collimating array which is optically coupled to the planarwaveguide.

At least one embodiment of the invention is configured as a method fordistributing radiant energy comprising: (a) receiving radiant energyinto an edge of an optical waveguide having edges disposed between afirst planar surface and a second planar surface; (b) propagating theradiant energy by optical transmission and total internal reflection inan optical material disposed between the first planar surface and thesecond planar surface along the length of the optical waveguide; (c)deflecting the radiant energy at a plurality of deflecting elementsdistributed along the first planar surface and/or second planar surfaceof the optical waveguide to a sufficiently low angle, below thepredetermined critical angle for total internal reflection (TIR) whichis with respect to a surface normal direction of the first planarsurface or second planar surface of the optical waveguide, causing theradiant energy to exit the surface of the optical waveguide through thefirst planar surface and/or the second planar surface; and (d)collimating the radiant energy exiting the optical waveguide at aplurality of focal zones in response to the radiant energy passingthrough a plurality of radiation collimating elements.

At least one embodiment of the invention is configured as an apparatusfor collecting light, comprising: (a) a plurality of light collectingelements within a collector array configured for collecting receivedlight; (b) a planar waveguide having edges disposed between a firstplanar surface and a second planar surface, in which the planarwaveguide is disposed in an optical receiving relationship with thecollector array and configured to propagate the received light byoptical transmission and total internal reflection; and (c) a pluralityof light deflecting elements optically coupled to the planar waveguidewith each of the plurality of light deflecting elements disposed inenergy receiving relationship within the planar waveguide to at leastone of the plurality of light collecting elements. Each of the lightdeflecting elements is configured to redirect incident light at asufficiently high angle, above the predetermined critical angle fortotal internal reflection (TIR) with respect to a surface normaldirection with respect to the first planar surface or the second planarsurface of the planar waveguide, to redirect and propagate the receivedlight within the planar waveguide by optical transmission and TIR.

In different embodiments and implementations the light collecting andlight deflecting elements can differ. In at least one embodiment, thelight collecting elements comprise a parallel array of elongated focusmirrors. In at least one embodiment, the light collecting elementscomprise a parallel array of elongated lenticular lenses. In at leastone embodiment, the light deflecting elements comprise a parallel arrayof elongated grooves. In at least one embodiment, the light deflectingelements comprise grooves within the planar waveguide configured forredirecting the received light in response to reflection from at leastone surface of the groove toward the collector array. In at least oneembodiment, the light deflecting elements comprise grooves formed withineach of a plurality of blocks that are attached and in opticalcommunication with the planar waveguide, and the grooves are configuredfor redirecting the received light in response to reflection from atleast one surface of the groove toward the collecting array. In at leastone implementation, the grooves are configured at a slope angle θ₃₀which is bounded by the relation

${\arcsin \left( \frac{n_{2}}{n_{1}} \right)} \leq \theta_{30} \leq {\arccos \left( \frac{n_{2}}{n_{1}} \right)}$

in which n₁ is the refractive index of the planar waveguide and n₂ isthe refractive index of an outside medium.

In at least one embodiment, the light deflecting elements are selectedfrom the group of optical elements consisting of planar mirrors, curvedmirrors, prisms, prism arrays, prismatic grooves, surface relieffeatures, reflective surfaces, refractive surfaces, diffractiongratings, holograms, and light scattering elements. In at least oneembodiment, the light collecting elements are selected from the group ofoptical elements consisting of imaging lenses, non-imaging lenses,spherical lenses, aspherical lenses, lens arrays, Fresnel lenses, TIRlenses, gradient index lenses, diffraction lenses, mirrors, Fresnelmirrors, spherical mirrors, parabolic mirrors, mirror arrays, and troughmirrors.

In at least one implementation, an optical interface layer is addedbetween the planar waveguide and the collector array, which preferablycomprises a lower refractive index (e.g., air, or other material) thanthe planar waveguide. In at least one implementation, the opticalinterface layer is selected from the group of optical materialsconsisting of low refractive index monomers, polymers, fluoropolymers,low-n optical adhesives, thin films, and optical waveguide claddingmaterials.

In at least one implementation, the planar waveguide comprises asubstantially rectangular plate having a first terminal edge, a secondterminal edge, a first side wall, a second side wall, a first planarsurface and a second planar surface. In at least one implementation, amirrored surface, or a cladding layer, is added on one or more of thefirst terminal edge, the second terminal edge, a first side wall or asecond side wall.

In at least one implementation, at least one optically responsiveelectronic device is coupled to at least one of the first terminal edgeor the second terminal edge of the planar waveguide. In at least oneimplementation, the electronic device can be optically coupled to acutout within the planar waveguide. In at least one implementation, anyoptional cladding or protective coatings are removed from the lightharvesting area, such as from the first or second terminal edge, and/orthe first or second side wall, to facilitate light transport andharvesting in the harvesting area.

In at least one implementation, both the collector array and the planarwaveguide have a round or sectorial shape obtainable by a revolution ofa cross section of the collector array and the planar waveguide aroundan axis.

In different implementations the collector array can be differentlyconfigured. In at least one implementation, the collector arraycomprises point focus lenses, or mirrors, which may have a shape such asround, rectangular, square, hexagonal, and so forth.

In at least one implementation, the planar waveguide and the collectorarray are adapted for being retained in either a planar configuration orin bent and/or rolled configurations.

In at least one implementation, the planar waveguide and collector arrayare adapted for being retained in a translated, a reversed and/or arotated orientation relative to each other toward adjusting theacceptance angle or for tracking the source of light. In at least oneimplementation, the planar waveguide and collector array are adapted forbeing retained in a movable relationship with one another adjusting theacceptance angle or for tracking the source of light. In at least oneimplementation, a coating is disposed on the exterior of said planarwaveguide and/or said collector array, such as including any of thefollowing coatings or combination of coatings thereof: anti-reflective,protective, encapsulates, reflective, diffusive, radiation protective,scratch and stain resistant, and light filtering.

At least one embodiment of the invention is configured as an apparatusfor collecting light, comprising: (a) a parallel collecting array havinga plurality of elongated light collecting structures configured forcollecting received light; (b) a planar waveguide having edges disposedbetween a first planar surface and a second planar surface, in which theplanar waveguide is disposed in an optical receiving relationship withthe collector array and configured to propagate the received light byelements of optical transmission and total internal reflection; and (c)a parallel deflecting array having a plurality of light deflectinggroove structures optically coupled to the planar waveguide with each ofthe plurality of light deflecting structures disposed in light receivingrelationship within the planar waveguide to at least one of the lightcollecting groove structures. Each of the plurality of light deflectinggroove structures is configured to redirect incident light at asufficiently high angle, above the predetermined critical angle fortotal internal reflection (TIR) with respect to a surface normaldirection of an exterior surface of the planar waveguide, to redirectand propagate the received light within the planar waveguide by opticaltransmission and TIR.

At least one embodiment of the invention is configured as a method forcollecting radiant energy comprising: (a) concentrating a radiant energyreceived upon a plurality of focal zones in response to a plurality ofradiation concentrator elements; (b) directing the radiant energy fromthe plurality of focal zones through a first planar surface into anoptical waveguide having edges disposed between a first planar surfaceand a second planar surface; (c) deflecting the radiant energy at aplurality of deflecting elements positioned to receive the radiantenergy from the focal zones, and to deflect the radiant energy into theplanar waveguide at angles exceeding the critical angle of totalinternal reflection in the waveguide, which is with respect to a surfacenormal direction of the first planar surface or second planar surface ofthe optical waveguide; and (d) propagating the radiant energy throughthe optical waveguide by optical transmission and total internalreflection.

The present invention provides a number of beneficial elements which canbe implemented either separately or in any desired combination withoutdeparting from the present teachings.

An element of the invention is an apparatus and method of collectinglight over a given area and traveling in a first direction, into awaveguide region directed in a second direction which can have anydesired angular relationship with the first direction.

Another element of the invention is the inclusion of distributeddeflecting means within the interior of the waveguide.

Another element of the invention is the coupling of a collimation means,such as a lens array, to the waveguide either directly, or with aninterposing material or air layer.

Another element of the invention is the use of reflective or refractivedeflecting means operating within the waveguide.

Another element of the invention is the use of deflecting elementsattached to the waveguide.

Another element of the invention is the use of deflecting elementsattached cut into the waveguide.

Another element of the invention is the use of deflecting elements whichextend from the waveguide.

Another element of the invention is the use of deflecting means havingat least one reflective or refractive, surface for redirecting the lightin relation to the waveguide.

Another element of the invention is the use of deflecting meanscomprising a facet containing both a reflective and transmissive surfacefor redirecting the light in relation to the waveguide.

Another element of the invention is the use of deflecting meanscomprising a facet containing both a reflective and transmissive surfacefor redirecting the light in relation to the waveguide.

Another element of the invention is the use of deflecting means whichmay be on the same, or opposite, side of the waveguide as thecollimating means.

Another element of the invention is the use of a linear array ofdeflecting and/or collimating means which span the surface of thedevice, or a portion thereof.

Another element of the invention is the use of separate deflectingand/or collimating means which are optically coupled to a specificdeflecting and/or collimating means.

Another element of the invention is a collimating means operating inresponse to refraction and/or reflection to direct light into or fromthe adjacent waveguide.

Another element of the invention is a light collimating or distributiondevice configured for performing light collimation on either side of thewaveguide device.

Another element of the invention is a light collimating and/ordistribution device which can be formed in a point form, linear form,annular form, as well as portions and combinations thereof.

Another element of the invention is a collimating and/or distributingdevice configured with an attached optically responsive device (e.g.,sensor) or optical illumination device.

A still further element of the invention is a light collection and/ordistribution device which can be utilized in a wide range of lightcollecting, light sensing, and light distribution applications.

Further elements of the invention will be brought out in the followingportions of the specification, wherein the detailed description is forthe purpose of fully disclosing preferred embodiments of the inventionwithout placing limitations thereon.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWING(S)

The invention will be more fully understood by reference to thefollowing drawings which are for illustrative purposes only:

FIGS. 1A and 1B are ray tracing diagrams for conventional lightcollection systems.

FIG. 2 is a schematic view and ray tracing of a compact light collectionsystem in accordance with at least one embodiment of the presentinvention.

FIG. 3 is a schematic view of the system shown in FIG. 2 according to atleast one embodiment of the present invention, showing a planar lensarray and prismatic grooved features.

FIGS. 4A and 4B are perspective views of a light collector according toat least one embodiment of the present invention.

FIG. 5 is a ray tracing diagram of compact light collection within FIG.4A, according to at least one embodiment of the present invention.

FIG. 6 is a ray tracing diagram of the compact light collection systemaccording to at least one embodiment of the present invention, depictedin greater detail.

FIG. 7 is a ray tracing of a first ray angle being trapped in awaveguide by means of TIR, according to at least one embodiment of thepresent invention.

FIG. 8 is a ray tracing of a second ray angle being trapped in awaveguide by means of TIR, according to at least one embodiment of thepresent invention.

FIG. 9 is a ray range tracing of light redirection from a first angularaperture to a second angular aperture, according to at least oneembodiment of the present invention.

FIG. 10A is a schematic of a waveguide portion comprising a block oftransparent material with a prismatic feature, according to at least oneembodiment of the present invention.

FIG. 10B is a schematic of a waveguide portion comprising a prismaticfeature protruding from a light conducting walls of a waveguide,according to at least one embodiment of the present invention.

FIG. 100 is a schematic of a waveguide portion having a bifacialprismatic grooved feature, according to at least one embodiment of thepresent invention.

FIG. 10D is a schematic of a waveguide portion incorporating a pluralityof prismatic surface relief features, according to at least oneembodiment of the present invention.

FIG. 10E is a schematic of a waveguide portion incorporating adiffraction grating for deflecting the light, according to at least oneembodiment of the present invention.

FIG. 11 is a ray tracing in response to a prismatic feature in a wall ofa waveguide according to at least one embodiment of the presentinvention.

FIG. 12 is a perspective view of a light collection device having acladding layer according to at least one embodiment of the presentinvention.

FIG. 13 is a ray tracing diagram of the collector shown in FIG. 12,according to at least one embodiment of the present invention.

FIG. 14 is a cross section view of a collector device coupled to aphotoresponsive device according to at least one embodiment of thepresent invention.

FIG. 15A through 15D are facing views of collector devices ofconfigurations according to different embodiments of the presentinvention.

FIGS. 16A and 16B are perspective views of an annular collectoraccording to at least one embodiment of the present invention.

FIG. 17 is a perspective view a light collector array according to atleast one embodiment of the present invention, showing the use of pointfocus lenses.

FIG. 18 is a top view of a light collector array according to at leastone embodiment of the present invention, showing a different arrangementof point focus lenses than were shown in FIG. 17.

FIG. 19 is a top view of a light collector array according to at leastone embodiment of the present invention, showing a different arrangementof point focus lenses than were shown in FIG. 17 and FIG. 18.

FIG. 20 is a perspective view of a plurality of deflecting means in apoint focus configuration on a waveguide according to at least oneembodiment of the present invention.

FIG. 21 is a ray tracing diagram of collection within a collector arrayformed by an array of micro-mirrors, according to at least oneembodiment of the present invention.

FIG. 22 is a ray tracing diagram of a lens array directly coupled to awaveguide and having a lower refractive index than the waveguide,according to at least one embodiment of the present invention.

FIGS. 23A and 23B are perspective views of the compact light collectionsystem according to at least one embodiment of the present invention,showing elongated (linear) deflectors and lenses operating incombination.

FIGS. 24 and 25 are ray tracing diagrams for conventional lightcollimation system.

FIG. 26 is a cross section view of a planar lens array and prismaticgrooved features shown operating within an illuminator according to atleast one embodiment of the present invention.

FIG. 27 is a detailed ray tracing diagram of the illuminator deviceshown in FIG. 26.

FIG. 28 is a detailed ray trace of light traversal through the waveguideof an illuminator according to at least one embodiment of the presentinvention.

FIG. 29 is a ray range tracing of light redirection from a first angularaperture to a second angular aperture within an illuminator according toat least one embodiment of the present invention.

FIG. 30A is a cross section view of a bifacial prismatic feature in awall of an illuminator waveguide, according to at least one embodimentof the present invention.

FIG. 30B is a cross section view of a multiple prismatic features in awall of an illuminator waveguide, according to at least one embodimentof the present invention.

FIG. 30C is a cross section view of a portion of an illuminatorwaveguide according to at least one embodiment of the present invention,showing use of a block of transparent material with a prismatic feature.

FIG. 30D is a cross section view of a portion of an illuminatorwaveguide according to at least one embodiment of the present invention,shown using a prismatic feature protruding from the waveguide.

FIG. 30E is a cross section view of a portion of an illuminatorwaveguide according to at least one embodiment of the present invention,showing utilization of a diffraction grating.

FIG. 31 is a ray tracing diagram of operation of an illuminatoremploying a prismatic groove formed in an opposing face of a waveguide,according to at least one embodiment of the present invention.

FIG. 32 is a ray tracing diagram of an illuminator employing a prismaticfeature protruding from an opposing face of the waveguide, according toat least one embodiment of the present invention.

FIG. 33 is a perspective view of an illuminator according to at leastone embodiment of the present invention, showing a material couplinglayer between the collimator and waveguide.

FIG. 34 is a cross section and ray tracing of a dual sided illuminatoraccording to at least one embodiment of the present invention.

FIG. 35 is a cross section and ray tracing of a combination illuminatordevice and light source, according to at least one embodiment of thepresent invention.

FIG. 36A through 36D is a facing view of illuminator arrays usinglenticular lenses, according to different embodiments of the presentinvention.

FIGS. 37A and 37B are perspective views of an annular illuminatoraccording to at least one embodiment of the present invention.

FIG. 38 is a detailed ray tracing of illuminator operation of acollector array formed by an array of micro-mirrors, according to atleast one embodiment of the present invention.

DETAILED DESCRIPTION OF THE INVENTION

Referring more specifically to the drawings, for illustrative purposesthe present invention is embodied in the apparatus generally shown inthe preceding figures. It will be appreciated that the apparatus mayvary as to configuration and as to details of the parts, and that themethod may vary as to the specific steps and sequence, without departingfrom the basic concepts as disclosed herein. Furthermore, elementsrepresented in one embodiment as taught herein are applicable withoutlimitation to other embodiments taught herein, and in combination withthose embodiments and what is known in the art.

1. Collector Embodiments

A wide range of applications exist for the present invention in relationto the collection of electromagnetic radiant energy, such as light.Therefore, for the sake of simplicity of expression, without limitinggenerality of this invention, the term “light” will be used hereinalthough the terms “electromagnetic energy” or “radiant energy” wouldalso be appropriate.

In order to be able to compare and contrast the present invention withtypical collectors, FIG. 1A and FIG. 1B are shown to illustrate theoperation of conventional light collection systems typically employing alarge-aperture optical collector device, such as lens 75 (FIG. 1A) or amirror 85 (FIG. 1B). Each lens 75 and mirror 85 can be characterized bya transversal size D and a focal length F. In the prior art, a radiationreceiver 45 is usually placed in the focus of the lens or mirror at aconsiderable distance from the collector. Rays 80 and 81 incident ontothe aperture of the collector are being directed to radiation receiver45. It will be appreciated by those skilled in the art, that in order toobtain useful light concentration, dimension D of the collector shouldbe significantly larger than the finite transversal size D_(S) ofradiation receiver 45. The focal length F, or the height of thecollector, also needs to be significantly greater than D_(S) for propercollection. The culmination of these dimensional relations requiressignificant system size and weight penalties which can be detrimental toimplementation in space constrained applications.

FIG. 2 illustrates a first embodiment 2 of a compact light collectingsystem. Light collection system 2 includes a planar collector array 5and a planar waveguide 4 configured to conduct light through it, such asalong and between its opposing parallel walls 10 and 11 by means ofoptical transmission and total internal reflection (TIR). The shape andlateral dimensions of collector array 5 approximate those of waveguide4. In at least one preferred embodiment, collector array 5 is disposedin close proximity to waveguide 4 so that the combination of collectorarray 5 and waveguide 4 form a planar sandwich-like configuration.

Collector array 5 comprises a plurality of light focusing means 6arranged in a planar array. Each focusing means 6 is configured toreceive an impinging beam of light, as may emanate from a distant lightsource (not shown), on its receiving surface in a pre-determinedacceptance angle and to focus this incident light onto a smaller focalarea so that collector array 5 forms a plurality of foci. The lightsource can be of any known type, including but not limited to sunlight,incandescent lamps, heat emitting bodies, light emitting diodes, lasers,light/heat scattering or radiating surfaces and the like. The incidentbeam can also be formed by an optical system providing a suitableangular and/or spatial energy distribution in the beam. For example, alight collimating device can be used to produce a generally parallelbeam of light that will impinge onto focusing means 6. In anotherexample, if the energy source is the sun, the incident light is aquasi-parallel beam of light in a broad spectrum of electromagneticspectrum. Collector array 5 is configured to have an entrance aperturefacing the light source and an opposing exit aperture facing waveguide4.

Focusing means 6 may comprise any desired optical structure adapted forcollecting or concentrating the impinging light. Any known opticalsystem or collector of radiant energy or light which collects the energyfrom a larger area and focuses it to a smaller focal area can be usedfor the purpose of this invention. By way of example and not limitation,focusing means 6 can be selected from the group of optical elementsconsisting essentially of spherical or aspherical refractive lenses,Fresnel lenses, TIR lenses, gradient index lenses, diffraction lenses,lens arrays, mirrors, Fresnel mirrors, mirror arrays and the like. Forthe purpose of this invention and from the practical standpoint, theterms “focal area” or “focus” of focusing means 6 should be understoodbroadly and generally refers to an area within the envelope of thefocused beam where said area has a cross section substantially smallerthan the cross section of respective focusing means 6. Accordingly, thefocal area can include areas at a relatively small distance from the“ideal” focus of focusing means 6 and where the focused beam can beconvergent (before focus) or divergent (after focus).

In accordance with this invention, it is preferred that an effectivefocal length of each focusing means 6 is substantially shorter than thedimensions of walls 10 and 11 in order to achieve better compactness ofsystem 2. For the purpose of this invention, the term “effective focallength” generally refers to the distance between focusing means 6 andits focus. This term should also be understood broadly and it alsoincludes the cases when the focal length of the same focusing means 6can change depending on the optical properties of the material fillingup the space between said focusing means 6 and the focus. In otherwords, the location of the effective focal area may be different (thusfocal length differs) when a different material separates lens 6 and itsfocal area. By way of example, for the same parameters of focusing means6, its focal distance can be longer in high refractive index material(e.g., polymethyl methacrylate (PMMA)) than in the air due to thedifference in refractive indexes.

Waveguide 4 is positioned in close proximity and generally parallel tocollector array 5 and is disposed in an energy receiving relationship,through transparent wall (face) 10, with respect to collector array 5.The energy receiving relationship is meant to mean any relationshipbetween waveguide 4 and collector array 5 which enables light to passfrom collector array 5 into waveguide 4. For this purpose, wall 10 ofwaveguide 4 is configured to transmit a substantial portion of lightincident onto the waveguide from collector array 5.

Waveguide 4 can be formed by any optically transmissive body having agenerally planar configuration and suitable for the purpose ofconducting electromagnetic radiation toward a terminal end or apre-determined portion of the waveguide by means of reflection of thepropagating light from the opposing walls. By way of example, it can bean optically transparent planar plate or a slab having a rectangular orcircular shape. Referring back to FIG. 2, an exemplary configuration ofwaveguide 4 comprises a substantially rectangular plate having lightconducting opposing walls 10 and 11 extending parallel to a predominantplane 9, a first terminal end wall 35, an opposing second terminal endwall 36, a first side wall and an opposite second side wall.

The thickness, or height, of waveguide 4 is selected to be substantiallyless than its lateral dimensions (length and width) so that the surfacearea of either planar wall 10 or 11 is substantially greater than thearea of at least one of the terminal walls 35 and 36. Further, waveguide4 is configured to be able to conduct light along and between at leastits light conducting walls 10 and 11 and generally toward at least oneof the terminal walls 35 and 36. A light harvesting area can beassociated with either of terminal walls 35 or 36 for collecting andconverting the light in whatever type of energy which is useful in theapplication. By way of example, waveguide 4 can be configured so that alight ray propagating in waveguide 4 at a normal angle to walls 10 and11 greater than a certain angle can be generally guided in one directiontoward the opposing face 36 by means of light conduction through thebody of waveguide 4, including bouncing of the light from faces 10 and11.

If used at optical frequencies, waveguide 4 can be made from adielectric, highly transparent material such as glass, PMMA, orpolycarbonate. In order to enhance its optical guiding ability, thematerial of waveguide 4 can be selected to have high index ofrefraction, and can be surrounded by a material with lower index ofrefraction.

It will be appreciated that the larger the incident angle from thesurface normal direction, the smaller is the fraction of lighttransmitted through the medium. Finally, at a sufficient angle from thenormal, a point of total internal reflection occurs, which is referredto as the TIR angle. At angles equal to or exceeding the TIR angle, allof the incident light is reflected back into the medium. Accordingly,the structure can guide optical waves in response to total internalreflection, characterized by a critical angle of TIR, so that when a rayof light propagating within waveguide 4 strikes a medium boundary (suchas wall 10 or 11) at an angle larger than the critical angle of TIR withrespect to the normal of the boundary surface plane, the ray isreflected back into the media of waveguide 4 so it can propagate furtherin said waveguide. Walls 10 and 11 should normally be smooth or polishedso as to avoid or minimize parasitic light scattering when undergoingTIR from said walls. When appropriate, wall 11 can be adapted with amirrored surface to enhance light guiding properties of waveguide 4.Additionally, the other walls of waveguide 4 can be made similarlysmooth and capable of reflecting light by means of TIR or specularreflection so that the light is kept within the waveguide even when itreaches either of the side walls. Wall 36 can also be made specularlyreflective in order to reflect any light arriving at it from the insideof waveguide 4 back into the waveguide. TIR reflectivity for either wallof waveguide 4 can be provided, for example, by making contact by thewall with a lower refractive index medium, such as the air, or byapplying a layer of a low-n cladding material to the wall. A specularreflectivity can be obtained in any desired manner, including but notlimited to the use of metallization, application of reflective films orother types of mirror finishing to further enhance the ability of thewaveguide to conduct light.

In accordance with at least one preferred embodiment, waveguide 4 shouldbe optically separated from collector array 5 by at least one opticalinterface 8 that provides trapping of the light propagating in thewaveguide after it has been deflected by deflecting means 14. Theprimary function of interface 8 is to allow light to enter waveguide 4from a variety of incidence angles and reject (by reflection) the lightcoming back out of waveguide 4.

A suitable optical interface 8 can be created by various mechanisms. Forexample, when the total internal reflection is used for trapping thelight in waveguide 4, interface 8 may comprise a physical boundary orwall of the body of waveguide 4 which is surrounded by outside mediawith lower refractive medium such as air. Alternatively, it can be aninterface between two media having different refractive indices so thatthe refractive index increases along the optical path from focusingmeans 6 toward waveguide 4. Interface 8 can be implemented by separatingwaveguide 4 from the body of collector array 5 or from bodies ofindividual focusing means 6 by means of a thin layer of air, a layer oflower refractive index dielectric medium or any other boundary between ahigher refractive index medium and a lower refractive index medium. In amore specific example, interface 8 can be implemented from an interfacebetween glass, PMMA or polycarbonate (high refractive index) and a lowrefractive index polymer or air. Alternatively, a layer of claddingmaterial can be provided between waveguide 4 and collector array 5 inwhich case, embodiment 2 of FIG. 2 can form a monolithic system whilemaintaining the same basic structure and operation. By way of exampleand in order to illustrate one or more of the preferred modes ofutilizing the present invention, interface 8 is formed by wall 10 ofhigh-refraction-index waveguide 4 and the surrounding ambientlow-refraction-index media (such as air) in FIG. 2.

Waveguide 4 comprises a plurality of light deflecting means 14associated with wall 11 and optically coupled to waveguide 4. The term“optically coupled” is directed to mean any relationship between twooptical components which enables light to pass from one opticalcomponent to the other. Deflecting means 14 can be any suitable opticaldevice used to receive the light beam in a pre-determined acceptanceangle from one direction and deflect at least a substantial portion ofthe incident beam from its original direction to a different direction.By means of example, deflecting means 14 can include a reflectivesurface or a refractive element or face disposed at an angle to theincident light beam. Similarly, deflecting means 14 can be selected fromthe group of deflecting means consisting essentially of planar mirrors,curved mirrors, mirror array, prisms, prism arrays, one or morereflective or refractive surfaces, diffraction gratings, holograms,light diffusing or scattering elements, and so forth.

The location of deflective means 14 in waveguide 4 and the position ofthe waveguide itself with respect to collector array 5 are interoperablyselected with each deflecting means 14 disposed at or near the focus ofone or more focusing means 6 (see FIG. 2). It is an important aspect ofthe present invention that the working area of light deflecting means 14is substantially smaller than the entrance aperture of the respectivefocusing means 6 illuminating said deflecting means 14. In other words,each focusing means 6 pre-concentrates the incident radiation from alarger area into a smaller focal area while the respective deflectingmeans 14 is configured to collect the concentrated light from the focalarea and redirect the light into waveguide 4 at a different angle thanthe angle of incidence. The light receiving surface, or entranceaperture, of each focusing means 6 should also be sufficiently spacedapart from the respective deflecting means 14 to allow for efficientfocusing of light. Yet, the distance between collector array 5 andwaveguide 4 should be kept small compared to the lateral dimensions ofcollector 2 toward enhanced system compactness.

Each deflecting means 14 is configured to receive the light beam whichis focused by focusing means 6 and redirect it into waveguide 4 at adifferent angle with respect to the angle of incidence. It is essentialthat at least a substantial portion of the redirected beam proscribe anangle with respect to surface normal of walls 10 and 11 greater than apre-defined critical angle θ_(C), so that the redirected radiationbecomes trapped in and propagated through waveguide 4 toward one or moreof its terminal ends.

TIR is one such convenient mechanism for trapping light in waveguide 4in which case critical angle θ_(C) can be selected to be the criticalTIR angle. It will appreciated by those skilled in the art of optics,that TIR can be defined as the reflection of electromagnetic radiationfrom an interface between a first and second optical medium in responseto an incident angle measured with respect to surface normal of theinterface. The first optical medium being more optically dense, andaccordingly having a higher index of refraction. It will also beappreciated that in response to TIR almost lossless internal reflectionsare provided.

According to Snell's law of optics, when light passes through a boundarybetween a first refractive medium and a second refractive medium, n₁ sinϕ₁=n₂ sin ϕ₂, where n₁ and n₂ are the refractive index of the firstmedium and the second medium, respectively, with ϕ₁ and ϕ₂ being theangle of incidence and the angle of refraction, respectively.Furthermore, the critical angle of TIR θ_(C) is the value of ϕ₁ forwhich ϕ₂ equals 90°. Accordingly, θ_(C)=arcsin (n₂/n₁·sin ϕ₂)=arcsin(n₂/n₁), which makes θ_(C) approximately 42.155° for an exemplary caseof the interface between PMMA (acrylic) with the reflective index n₁ ofabout 1.49 and air with n₂ of about 1.

As discussed above, the condition of TIR at wall 10 can be achieved byproviding the refractive index of waveguide 4 which is greater than therefractive index of the outside media contacting waveguide 4 at wall 10.Wall 11 can also be configured to contact an outside media having alower refractive index than the refractive index of waveguide 4 to allowfor reflecting the light trapped in waveguide 4 by means of TIR.Alternatively, or in order to improve the reflection of light from wall11 in a broad range of angles and/or wavelengths, wall 11 can bemirrored to provide for specular reflection. Mirrored surface of wall 11can be obtained by depositing a reflective layer using any known means,such as, for example, silvering, aluminizing or laminating with amirrored film.

In operation, as illustrated in FIG. 2, the collector device can be usedto collect a distributed beam of light by a larger entrance aperture ofcollector array 5 and concentrate the collected energy on the smallerexit aperture of a first terminal end wall 35 of waveguide 4. Eachdeflecting means 14 receives a focused light beam (illustrated as anincoming fan of rays) formed by focusing means 6 and injects the focusedlight beam into waveguide 4 at a sharper angle with respect to bothwalls 10 and 11 (the injected light beam is shown as an outgoing fan ofrays in FIG. 2) to provide that the TIR condition is met for each ray inthe injected light beam. As discussed above, wall 36 which is oppositeto first terminal end wall 35, can be mirror coated to reflect any light(e.g., stray light) back into waveguide 4 and toward wall 35. Thedimensions of waveguide 4 are selected so that area of wall 35 issubstantially smaller than the area of collector array 5 and wall 10 ofwaveguide 4. In this case, the light injected into wave guide throughthe large surface area of wall 10 will arrive at wall 35 with a greaterlight intensity compared to the intensity found at wall 10. Assuming anideal case of negligible optical losses in waveguide 4, a geometricalconcentration ratio C_(G) can be found from the following formula:

${C_{G} = \frac{S_{IN}}{S_{OUT}}},$

where S_(IN) is the area of wall 10 and S_(OUT) is the area of wall 35.In an exemplary case of a 5 mm thick rectangular waveguide 4 havingdimensions of wall 10 of about 20 cm by 10 cm and dimensions of wall 35of about 10 cm by 0.5 cm, C_(G) will be approximately equal to

$\frac{20\mspace{14mu} {cm} \times 10\mspace{14mu} {cm}}{10\mspace{14mu} {cm} \times 0.5\mspace{14mu} {cm}} = 40.$

This means that the average light intensity at wall 35 will beapproximately 40 times greater than the average light intensityimpinging on the entrance aperture of collector array 5 or wall 10 ofwaveguide 4. The concentrated light received at wall 35 can be furtherdirected, extracted from waveguide or converted to any desired form ofenergy or signal. For this purpose, wall 35 can be configured astransparent and/or can be associated with a light detector or energyconversion device. Alternatively, the wall can be configured to allowfor ejecting the concentrated light out of waveguide 4 through walls 10or 11. For this purpose, wall 35 can be mirrored and inclined at anangle with respect to a surface normal direction of either wall 10 or 11(for example at an angle of about 45 degrees) thus allowing the lightarriving at wall 35 from the inside of waveguide 4 to be reflected fromwall 35 and extracted from waveguide 4 toward a perpendicular to plane9.

By way of a further example and taking an illustrative case of agenerally parallel beam emanated by a distant source subtending arelatively small finite angle (such as the beam produced by sunlight ora distant light emitting device), collector array 5 can be designed as aplanar lens array.

FIG. 3 illustrates an example implementation of embodiment 2, in whichcollector array 5 comprises a planar lens array where the plurality ofcollecting means (elements) 6 are each represented by a positive lens(collecting/concentrating) disposed in a planar configuration. Thelenses forming the planar lens array can be of any desired configurationwhich provides for concentration of the received light, including butnot limited to lenticular, cylindrical, round, hexagonal, square,rectangular, linear-focus, or point-focus lenses, and can be packed withany desired density covering the entrance aperture of collector array 5.The lens array can be fabricated using any conventional method such asreplication, molding, micro-machining, chemical etching, beam etchingand the like. The individual lenses can be integrated with collectorarray 5 and preferably comprise the same material as the body of thearray. Alternatively, the lens array can be disposed on a transparentsubstrate plate and fabricated of the same or a different material thanthe substrate plate. Individual lenses can also be configured asseparate pieces and attached to the substrate plate. Suitable materialsinclude but are not limited to optical glass, polymethyl methacrylate(PMMA), silicone, polycarbonate, polystyrene, polyolefin, any opticallyclear resin which is obtainable by polymerization and curing of variouscompositions, and other methods directed at creating a sufficientlyoptically transparent structure. The placement of lenses in the lensarray can be according to any suitable spatial metric and by any desiredmeans. For example, the lenses can be spaced apart, contacting eachother or overlapping and can be positioned in any desired pattern in theplanar array.

For the purpose of illustrating the present invention, the lens array isselected to be a densely packed lenticular lens array in which eachcollecting means 6 is represented by a cylindrical lens. Each lens isdesigned to have a point of focus located outside of the lens arrayitself, preferably at a pre-determined distance from the lens array,such as at a deflector positioned on an opposing side of a waveguidehaving a given refractive index. Accordingly, when positioned with oneside representing the entrance aperture perpendicular to the incidentbeam, the planar array of collecting means 6 provides a plurality offoci on the opposite side, the foci being spaced apart from each otherin accordance with the spacing of individual lenses in the lens array.With the lens array being planar and individual lenses having anidentical optical configuration, the plurality of foci of individualreflecting means 6 provides a common focal plane disposed at a distancefrom lens array 5.

Referring to FIG. 3, waveguide 4 is shown comprising a substantiallyplanar light guide formed by a transparent plate having a rectangularshape and configured to conduct light by means of TIR along its parallelfaces 10 and 11. Waveguide 4 comprises a plurality of deflecting means14 associated with wall 11, each deflecting means 14 being designed as aparallel grooved structure formed by a tapered prismatic void, V-shapedgroove or micro-prism in wall 11, the grooved structure having at leastone sloped reflective face. The elongated parallel grooved structuresforming deflecting means 14 should preferably have the same spacing andapproximately the same extent as the parallel lenticular lenses formingfocusing means 6. A “V”-shaped groove can be either symmetric orasymmetric and having faces which can make any suitable individualangles with wall 11.

A variety of methods can be utilized for incorporating the prismaticgrooved structures within wall 11 to create the surface reliefmicro-structures or texture described. By way of example, the structurescan be fabricated using a technique for direct material removalincluding mechanical scribing, laser scribing, micromachining, etching,grinding, embossing, imprinting from a master mold, photolithography,and a plurality of known methods and combinations thereof forstructuring optical materials. In addition, the faces of prismaticgrooved structures can be optionally polished, as desired, to obtain anydesired level of polished smooth surface. Alternatively, waveguide 4 canbe fabricated to incorporate embedded grooves, such as by means ofcasting, injection molding, compression molding, or similar processesand combinations of molding and machining processes thereof.

Alternatively, waveguide 4 can incorporate a layer of transparentmaterial, such as a plastic film or thin transparent plate, attached toface 11 and the prismatic grooved structures can be formed in thatlayer. Various mechanisms, including optical lithography, can be used tocreate the required pattern in a light-sensitive chemical photo resistby exposing it to light (typically UV) either using a projected image oran optical mask with the subsequent selective removal of unwanted partsof the thin film or the bulk of a substrate.

In a further alternative, the transparent material can be overmoldedonto waveguide 4 in the respective areas and prismatic groovedstructures can be formed in the over mold. By way of example, and notlimitation, a negative replica of the grooves can be formed by diamondcutting/machining, laser micromachining, ion beam etching, chemicaletching, or similar techniques followed by imprinting of it in theovermold. In the illustrated case, deflecting means 14 is formed byprismatic grooved structures in face 11 to extend end-to-end across oneface of waveguide 4 and to be optically coupled with waveguide 4directly through its surface, without the need of any additional opticalinterfaces or layers and their attendant optical losses.

Waveguide 4 is preferably positioned parallel to collector array 5, andis shown directly underneath it in the figure, so that the plurality ofdeflecting means 14 is disposed in the focal plane of the lens array. Inat least one embodiment a thin cushion layer, or space, is providedbetween collector 5 and waveguide 4. The thickness of waveguide 4 andthe cushion space are so selected in relevance to the focal length ofindividual lenses of collector array 5 that each deflecting means 14 islocated in a focal area of the respective collecting means 6 so thateach lens representing collecting means 6 can focus the incident lightonto the reflective face of the respective prismatic groove representingdeflecting means 14. Thus, the array of collecting means 6 is configuredto have a matching array of deflecting means 14 positioned in thevicinity of the focal plane of the lens array. However, it should beunderstood that deflecting means 14 can be positioned with anypredefined offset from the focus or they can also be positioned in aconvergent or divergent beam provided that light collecting system 2 hasthe same basic arrangement. Each deflecting means 14 is adapted with afirst face for deflecting light received from collecting means 6, whilea second face (shown as a vertical step in the figure) can be adapted asdesired to enhance the characteristics of light passing throughwaveguide 4. By way of example and not limitation, the second face ofdeflecting means 14 can be sloped (not shown), at any desired angle,such as even reaching the base of the preceding deflecting means, or anyintermediate position, so as to reduce backscatter and maximize lighttransmission through the waveguide.

In at least one embodiment of FIG. 3, waveguide 4 comprises a highlytransparent material having a refractive index n₁ which should begenerally greater than a refractive index n₂ of the outside medium(n₁>n₂). In an exemplary case of waveguide 4 being made from glass orPMMA, n₁ is about 1.5. The thin cushion space between collector array 5and waveguide 4, provides a thin layer of a low refractive indexmaterial, exemplified as air which has a refractive index of aboutunity. As a result, the refractive index increases outwardly at eachexternal face of waveguide 4 including walls 10 and 11. Walls 10 and 11serve as TIR reflectors for light propagating in waveguide 4 at angleswith respect to a surface normal direction with respect to walls 10 and11 at greater than θ_(C). As discussed above, θ_(C) is, in this case, acritical angle of TIR and wall 10 also serves as the light trappingoptical interface 8 between waveguide 4 and focusing means 6.

Referring yet further to FIG. 3, the reflective face of each groovedstructure is inclined at a sufficient angle with respect to wall 11 sothat it deflects the focused beam formed by respective collecting means6 back into waveguide 4 at an angle allowing for the propagation of thereflected beam by optical transmission and by means of TIR from walls 10and 11 toward terminal end 35 of waveguide 4. The reflective faces ofthese grooved structures can be metalized or otherwise configured with ahighly reflective surface.

For the sake of illustrative clarity, only four focusing means 6 andfour matching deflecting means are shown in FIG. 2 and FIG. 3; however,it should be understood that collector array 5 can incorporate anysuitable number of focusing means 6 to provide for a desired operationand light collection and that waveguide 4 can also incorporate anysuitable number of deflecting means 14 in order to trap the light beamsformed by collector array 5 into the waveguide.

In addition, the thickness of collector array 5 and waveguide 4 isexaggerated in FIG. 2 and FIG. 3 for the sake of illustrative clarity.However, it should be understood that either, or both, collector array 5and waveguide 4 may comprise layers of any desired thickness, such asimplemented as sufficiently thin layers to result in creating a verycompact planar device. The size of deflecting means 14 is alsoexaggerated for clarity; however, it should be understood that theindividual deflecting means 14 require a substantially smallerreflecting surface than the size of the respective focusing means 6 fromwhich light is directed onto the reflecting surface. Accordingly, lightis injected into waveguide 4 through a plurality of small-area zones,which reduce the chance for a light ray deflected by an individualdeflecting means 14 to enter into such a zone a second time on its wayin waveguide 4 and therefore to reduce interception of light alreadytrapped in waveguide 4 toward maximizing system throughput andefficiency. Accordingly, the relative dimensions of waveguide 4 anddeflecting means 14 are also selected so that the projected area ofdeflecting means 14 in the path of light propagating in waveguide 4 issubstantially smaller than the transversal cross section of thewaveguide 4 in the path of light. In other words, the area of eachdeflecting means 14 should be sufficient to intercept a substantialportion of light focused by respective focusing means 6, but a crosssection of the deflecting means 14 in a plane perpendicular to theprevailing direction of light propagation in waveguide should besubstantially smaller than a cross section of waveguide 4 in the sameplane. This can be necessary especially in the case of lenticularconfiguration of collecting means 6 and deflecting means 14 in order tominimize the light blockage or other interference of deflecting means 14with the light trapped in waveguide 4 by other deflecting means 14 andpropagating along the waveguide toward a pre-determined direction.

In reference to the example embodiment of FIG. 3, this minimization oflight blockage is by selecting the depth of grooved structures to besubstantially smaller than the thickness of waveguide 4, the thicknesscan be defined in relation to the distance between faces 10 and 11. Itwill be appreciated by those skilled in the art that the interference ofdeflecting means 14 with light propagating in waveguide 4 can beminimized by minimizing the depth of the receiving aperture ofindividual deflecting means 14 and by positioning the deflecting meansdirectly in the focus or a close proximity of the focus of respectivecollecting means 6. In certain instances, for example when theacceptance angle of system 2 needs to be increased, the receiving area(and hence the overall size) of deflecting means 14 can be made slightlylarger than the cross section of the effective focal area of therespective collecting means 6. In this case, deflecting means 14 willaccept focused light from a broader range of angles while notsubstantially impairing the light throughput of waveguide 4. Since apoint-focus lens or any other conventional light collector usuallyproduces a much smaller focal area than a linear focus configurationwith the same cross sectional design of the collector, it will also beappreciated by a skilled artisan in the subject field that the size ofdeflecting means 14 can also be minimized by selecting a point-focusconfiguration for each collecting means 6 versus its linearconfiguration.

FIG. 4A-4B illustrate the exemplary linear configuration of thecollector device in FIG. 3, showing a first perspective view in FIG. 4Aof the top-side, and a perspective view in FIG. 4B of the device afterbeing rotated upside down. Collector array 5 comprises a lenticular lensarray having a rectangular shape and waveguide 4 comprises a rectangulartransparent plate preferably having the same length and width as thelens array, with end walls (terminal sides) 35, 36, and side walls 40,41. In FIG. 4A, deflecting means 14 are shown implemented as linearprismatic grooves in wall 11 of waveguide 4, the prismatic grooves beingaligned parallel to the longitudinal axes of respective lenticularlenses of the collector. In such a linear configuration of collectingmeans 6, it is preferred that deflecting means 14 have about the sameextent as the respective collecting means 6 in order to intercept theentire focused beam.

FIG. 4B shows a different view of system 2 shown in FIG. 4A. Thewaveguide structure and its prismatic grooves can be fabricated by anydesired method, including without limitation, etching, grinding,scribing, extrusion, embossing, imprinting from a master mold, injectionor compression molding, other conventional methods, and combinationsthereof. The grooves can extend as desired across a face of waveguide 4from first side wall 40 to opposing second side wall 41, or anysubstantial portion thereof, so that the base of such a groove can forma rectangular opening in wall 11 with a triangular cross section, asillustrated in FIG. 4B. As discussed above, the transverse size ofdeflecting means 14 is exaggerated for clarity. Waveguide 4 can also beimplemented with grooves already embedded into it by means of casting,injection molding, compression molding or similar processes.Alternatively waveguide 4 can incorporate a layer of transparentmaterial, such as a plastic film or thin transparent plate, attached towall 11 and the prismatic grooves can be formed in that layer.

Waveguide 4 is spaced apart from collector array 5 and thus is separatedfrom the collector array by a layer of air or other media with a lowrefraction index compared to the material of waveguide 4. Walls 10 and11 are thus disposed in direct contact with air and can conduct light byoptical transmission and TIR. Accordingly, each prismatic groove isdisposed along the focal line of a respective linear lens and has asloped reflective face that is capable of intercepting the focused lightbeam from the lens and redirecting the light beam into waveguide 4 at anangle allowing for TIR on walls 10 and 11.

In FIG. 4A, an incident light ray 30 enters one of the focusing means 6and is directed by it down to one of deflecting means 14 disposedparallel to the focusing means 6 and configured to redirect ray 30 backinto the waveguide but away from the original propagation path of ray30. In the illustrated case when deflecting means 14 is formed by aprismatic grooved feature in wall 11 of waveguide 4, a reflective faceof the grooved feature is inclined at a suitable angle with respect towall 11 to result in the angle that ray 30 makes with surface normal towall 10 being greater than critical angle θ_(C). For the purpose ofillustrating this invention, θ_(C) is selected to be the critical angleof TIR at the interface formed by wall 10 with the outside media.Focusing means 6 and respective deflecting means 14 are also oriented todirect ray 30 generally toward wall 35. The extent to which anindividual deflecting means 14 extends in waveguide 4 is indicated by adotted line. A portion of ray 30 propagating inside system 2 and itscomponents such as collector array 5 and waveguide 4 is indicated by adashed line. After being redirected by deflecting means 14, ray 30propagates in waveguide 4 by striking wall 10. Since the requirement ofTIR is met, ray 30 upon striking wall 10 is reflected back intowaveguide with a negligible loss. As a matter of optics, ray 30 isreflected from wall 10 by means of TIR at the same angle with respect toa normal to wall 10 as it makes with the normal upon striking wall 10.Consequently, upon bouncing from wall 10 by means of TIR, ray 30 furtherpropagates in waveguide 4 and strikes wall 11. Since wall 11 is parallelto wall 10, a normal to wall 10 is also a normal to wall 11 and therequirement of TIR is also met for the interface formed by wall 11 andthe outside media. Accordingly, ray 30 undergoes TIR at wall 11 with alow loss and maintains the same angle to a normal to wall 10 and 11. Ray30 is thus trapped by TIR within waveguide 4 and propagates through thewaveguide toward a terminal end at wall 35. Depending on theapplication, ray 30 can further cross wall 35 and enter, for example, alight detector or an energy conversion device adjacent to wall 35.

FIG. 5 illustrates an example of light rays passing through thecollector and being retained by TIR within the waveguide according tothe present invention. As shown in FIG. 5, a ray R₁ is received from asubstantially parallel light source (e.g., a distant light source) as itstrikes the entrance aperture of the collector array, and moreparticularly, the entrance aperture of an individual focusing means 6.Focusing means 6 is shown implemented as a positive cylindrical lenswhich refracts ray R₁ and redirects it toward the focal area of thelens. Ray R₁ crosses wall 10 of waveguide 4 with some refraction andstrikes light deflecting means 14 disposed in the vicinity of the focusof focusing means 6. Deflecting means 14 redirects at least asubstantial portion of energy of ray R₁ into waveguide 4 by means ofreflecting ray R₁ from a sloped reflective face of the prismatic groove.Waveguide 4 has a higher refractive index n₁ than the surrounding medium(n₂). The angle with respect to a normal to waveguide 4 at whichdeflecting means 14 reflects ray R₁ into waveguide 4 medium is equal orgreater than critical angle θ_(C) defined by a critical angle of TIRwhich, in turn, is defined by refractive indices n₁ and n₂.

In similar manner, a ray R₂ impinging onto the receiving surface offocusing means 6 is directed to the same focal area and to the samelight deflecting means 14. Ray R₂ enters focusing means 14 at adifferent angle than ray R₁ but is further redirected into waveguide 4so that ray R₂ also propagates in the medium of waveguide 4 at an anglegreater than θ_(C) that permits for a total internal reflection fromwalls 10 and 11. Similarly, rays R′₁ and R′₂ focused on a differentreflecting means 14 by the respective collecting means 6 are alsoreflected into waveguide at angles allowing for propagating thereflected rays in waveguide 4 by means of TIR.

It should be understood that while the figure depicts only two examplerays, focusing means 6 is configured to collect any rays impinging ontoits receiving aperture in a pre-defined acceptance angle and anydesirable spectral range. While only parallel rays impinging onto thereceiving aperture of collector array 5 are shown in FIG. 5, it shouldalso be understood that, deflecting means 14 can be configured toreceive a convergent or divergent beam of light having a predeterminedangular spread and redirect the beam to waveguide 4 at a sufficient bendangle so that each ray of the redirected beam becomes trapped inwaveguide 4 and further propagates within the waveguide 4 by means ofTIR from walls 10 and 11. It will be appreciated by those skilled in theart that collector array 2 can operate with any number of rays within aselected acceptance angle and in a desired spectral range of theincident light. Particularly, collector array 2 can be used toconveniently inject a quasi-parallel beam of monochromatic orbroad-spectrum electromagnetic energy into waveguide 4 through alarge-area light conducting wall of the waveguide as opposed toinjecting the beam through a terminal end of the waveguide as withinconventional devices.

FIG. 6 illustrates a ray traversing waveguide 4 in further detail byshowing and analyzing a path of ray R₁. Referring to FIG. 6, ray R₁directed by a focusing means (element) is propagated in the lowerrefractive index medium surrounding waveguide 4 crosses wall 10 ofwaveguide 4 and further propagates in the higher refractive index mediumof the waveguide until it strikes light deflecting means 14. Lightdeflecting means 14 is designed to deflect ray R₁ from its originaldirection of propagation in waveguide 4 into a different direction. Inorder to do this, a reflective face 26 is provided in light deflectingmeans 14. Reflective face 26 is inclined with respect to wall 11 so thatit makes a slope angle θ₃₀ with wall 11 and an angle θ₃₅ with a surfacenormal direction 15. If θ₃₉ is an angle between face 26 and ray R₁, thenθ₃₉=θ₃₅−θ₃₀. Face 26 has a planar mirrored surface to provide for alow-loss specular reflection. Reflective face 26 is illustrated to havea planar surface. However, it should be understood that face 26 can beadapted with reflective surfaces other than planar surfaces, for examplesegmented, curved surfaces. It will also be appreciated that althoughthe back face of deflecting means 14 is shown following the surfacenormal direction, it can be configured at a desired slope back towardthe previous deflector, for reducing back scatter of rays traversing thewaveguide.

Upon incidence onto face 26 at point P₁ an angle θ₁, ray R₁ reflects atan angle θ₂ with respect to a surface normal direction 15 to wall 10.The corresponding portion of ray R₁ propagating from wall 10 to lightdeflecting means 14 is denoted as a ray segment 17. A ray segment 18represents a continuation of the ray R₁ when it is internallyredirected/deflected by deflecting means 14 back into waveguide 4 but ata different angle so that segment 18 forms an angle θ₂ with respect to anormal to wall 10. The slope of face 26 is selected so as to result inangle θ₂ being greater than angle θ₁ and equal to or greater than angleθ_(C). As discussed above, angle θ_(C) can be defined from the followingexpression for a critical TIR angle:

θ_(C)=arcsin(n ₂ /n ₁),

where n₁ and n₂ are the refractive indices of waveguide 4 and the lowerrefractive index medium adjacent to wall 10 of waveguide 4,respectively.

When ray R₁ is reflected by face 26 and further strikes wall 10 from theinside of waveguide 4 at point P₁, it makes an angle of incidence withrespect to the surface normal direction of interface wall 10. Obviously,the angle of incidence is equal to θ₂ due to the parallelism of walls 10and 11 and surface normal direction 15 to wall 10 is also a normal towall 11 for the same reason. Since angle θ₂ is greater than angle θ_(C),the condition of TIR is automatically met for wall 11. Therefore, ray R₁does not pass through wall 10 and is totally internally reflected backinto waveguide 4 maintaining the same angle θ₂ with respect to a normalto walls 10 and 11. As a result, ray R₁, after being deflected by lightdeflecting means 14, will become trapped in waveguide 4 and willcontinue to propagate in waveguide 4 by bouncing from walls 10 and 11due to TIR. The above condition can be achieved by providing a suitableangle between a normal to sloped reflective face 26 and surface normaldirection 15 so as to allow for sufficient bend angles for rays focusedby focusing means 6.

Referring further to FIG. 6, since surface normal direction 15 makes anangle of 90° with walls 10 and 11, θ₃₅=90°−θ₃₀. The following expressioncan also be derived as a matter of optics and geometry:θ₂=2(90°−θ₃₅)+θ₁. Thus, for the example illustrated in FIG. 6, if ray R₁enters waveguide 4 so that it makes an angle of 10° with respect tonormal 15 at point P₁, that is θ₁=10°, and face 26 is inclined at anangle of 27° with respect to wall 10, that is θ₃₀=27° and θ₃₅=63°, thena value θ₂=64° is obtained. This means that segment 18 will strike wall10 at the angle of 64° with respect to a normal of wall 10. If waveguide4 is made from PMMA with the reflective index n₁ of about 1.49 and theambient medium is air with refractive index n₂ of about 1, angle θ_(C)selected in this case to be the TIR angle will be equal to arcsin(1/1.49) which is approximately 42.155°, that is greater than angle θ₂.Thus, it follows that, in the above example, θ₂>θ_(C). Therefore thecondition of TIR is met at point P₂ and that ray R₁ will undergo a totalinternal reflection at wall 10. Since ray R₁ maintains the same anglewith respect to a normal to parallel walls 10 and 11 when subsequentlybouncing from the walls, the condition or TIR is also preserved alongthe entire length of waveguide 4. Thus, ray R₁ becomes trapped inwaveguide 4 so it can propagate along its walls 10 and 11 toward aterminal end. In another example, if ray R₁ enters waveguide 4perpendicular to wall 10 (i.e., θ₁=0°) and face 26 is inclined at anangle 45 degrees with respect to wall 10 and normal 15 (θ₃₀=45° andθ₃₅=45°), θ₂=90°, which means that segment 18 is perpendicular to normal15 and parallel to both walls 10 and 11. Therefore, in this latterexample, R₁ will propagate in waveguide 4 toward a terminal end withouttouching either wall 10 or 11.

FIG. 7 illustrates an example ray diagram which illustrates that byselecting a suitable slope angle θ₃₀ of reflective face 26, ray R₁ canbe directed at any desired angle with respect to surface normaldirection 15 or walls 10 and 11. The figure illustrates this exemplarycase when reflective face 26 is inclined at a greater angle θ₃₀ withrespect to wall 11 so that at least a portion of light redirected bydeflecting means 14 can strike wall 11 first. In FIG. 7, ray R₁ enterswaveguide 4 and propagates in it so that segment 17 makes angle θ₁ withsurface normal direction 15. Ray R₁ strikes reflective face 26 ofdeflecting means 14 and is reflected into waveguide 4 so that segment 18makes an angle θ₂ with respect to surface normal direction 15. Slopeangle θ₃₀ is selected to result in angle θ₂ being greater than θ_(C).Accordingly, upon striking wall 11 at point P₂, ray R₁ makes an angle ofincidence equal to θ₂ which is greater than the TIR angle. Since walls10 and 11 are parallel, a TIR will occur each time when ray R₁ strikeseither of the walls. Accordingly, ray R₁ becomes trapped in waveguide 4and can propagate along its walls 10 and 11 by means of at least TIR.

FIG. 8 illustrates another ray path R₂ in the system depicted in FIG. 7.Ray R₂ propagates in waveguide 4, as indicated by a ray segment 31 andimpinges onto face 26 at an angle of incidence θ₄₁. Segment 31 makes anangle θ₄ with respect to surface normal direction 15. A ray segment 32represents a continuation of ray R₂ when it is reflected from face 26back into waveguide 4. Angle θ₄₁ is greater than angle θ₂₉ of FIG. 7resulting in the bend angle of ray R₂ in FIG. 8 being greater than thatof ray R₁ in FIG. 7. Slope angle θ₃₀ of face 26 is selected so thatsegment 18 makes an angle θ₅ which is greater than angle θ₄, while angleθ₅ is greater than a TIR angle θ_(C). Accordingly, the condition of TIRpropagation in waveguide 4 is satisfied for ray R₂ and it can alsopropagate along walls 10 and 11 toward a terminal end.

Reflective face 26 can be inclined at an even more acute angle withrespect to surface normal direction 15 in which case it can reflect aportion or all incident focused beam by means of TIR in which case nomirror coating may be required for face 26. Referring to FIG. 7, anangle θ₂₉ represents an angle of incidence of ray R₁ onto face 26 withrespect to a surface normal direction 28. When face 26 makes asufficient angle with respect to segment 17, angle θ₂₉ can exceed a TIRangle for the optical interface formed by face 26 and the outside media.Thus, ray R₁ will undergo TIR at face 26 even if face 26 is opticallytransparent and not specularly reflective.

FIG. 9 illustrates by way of example, both incident and reflected beamranges from the surface of deflector 14. In considering an individualdeflecting means 14, the focused beam impinging onto face 26 can becharacterized by a cone of light having a first angular aperture A₁ asseen in the figure. As discussed above, deflecting means 14 can beconfigured to receive light rays incident into its working surface atdifferent angles and to redirect the rays at angles greater than the TIRangle in relation with walls 10 and 11. Thus, deflecting means 14 can beconfigured to receive light from first angular aperture A₁ and redirectthe light into a second angular aperture A₂ so that apertures A₁ and A₂do not intersect, and each ray in the second angular aperture A₂propagates at an angle with respect to surface normal direction 15greater than angle θ_(C). When deflecting means employ a planarreflective face 26, the angular value of second angular aperture A₂ willgenerally be the same as the angular value of first angular aperture A₁.However, face 26 can also be made concave or convex resulting in thesecond angular aperture A₂ being greater or smaller than first angularaperture A₁. Since a light ray striking wall 10 from the outside ofwaveguide 4 cannot practically enter the waveguide at an angle withrespect to surface normal greater than θ_(C), a practical limit for A₁is defined by the refractive indices of waveguide 4 and the outsidemedium: A₁≤2θ_(C) or A₁≤2 arcsin (n₂/n₁). When A₁=2θ_(C), in view ofminimizing losses of light coupling to waveguide 4, a practical usefulrange for slope angle θ₃₀ can be defined from the followingrelationship: θ_(C)≤θ₃₀ 90°−θ_(C) or

${\arcsin \left( \frac{n_{2}}{n_{1}} \right)} \leq \theta_{30} \leq {{\arccos \left( \frac{n_{2}}{n_{1}} \right)}.}$

By taking an above exemplary case of waveguide 4 being made from PMMA(n₁≈1.49) with air cladding (n₂≈1), the desired range for slope angleθ₃₀ is obtained as: 42.16°≤θ₃₀≤47.84° which provides a slope angle widthof about 5.7° for obtaining the maximum light coupling efficiencyemploying prismatic grooved features for deflecting means 14.

In a more general case, and when first angular aperture A₁ is less than2θ_(C), a practical range of useful slope angles θ₃₀ can be defined asfollows: A₁/4+θ_(C)/2≤θ₃₀≤90° −A₁/4−θ_(C)/2. If slope angle θ₃₀ isoutside of this range, a portion of the light beam redirected by therespective prismatic groove 14 may exit from waveguide 4 through one ofits light conducting walls 10 or 11 and that decoupled light will belost.

It should be appreciated that although FIG. 4 through FIG. 8 illustratedembodiments which employ a light deflecting means 14 formed by a groovedstructure associated with wall 11 of waveguide 14 and having slopedreflective face 16, the invention is not limited to this configuration.Specifically, light deflecting means 14 can be positioned anywhere at orbetween walls 10 and 11, and can be configured as embedded or integralto waveguide 4 or attached externally to either wall 10 or 11, providedthat the deflecting means 14 is optically coupled to waveguide 4 and canintercept the focused beam from the respective focusing means 6 andinject the beam into the waveguide at an angle allowing for lighttrapping by means of at least TIR.

FIG. 10A through FIG. 10E illustrate, by way of example and notlimitation, alternative implementations of light deflecting means 14disposed on surface 11. It should be noted that each of these variationscan be implemented separately or in combination with one another withoutdeparting from the teachings of the present invention.

In FIG. 10A, deflecting means 14 comprises a block of transparentmaterial attached to wall 11 and optically coupled to waveguide 4. Inthis case, deflecting means 14 can have a prismatic relief feature witha reflective face 26 which is capable of redirecting a focused beam oflight into waveguide at an angle θ₂ greater than θ_(C). The material ofdeflecting means 14 can be selected to approximately match that ofwaveguide 4 in which case the parasitic reflections at the interfacebetween waveguide 4 and deflecting means 14 can be minimized whichminimizes the losses related to light propagation both to and fromdeflecting means 14.

FIG. 10B illustrates a further example in which a deflecting meanscomprising a prismatic feature is protruding from face 11. In thisexample, reflective face 26 is provided so that system 2 has the samebasic operation as described above as one can see the tracing of ray R₁.

FIG. 100 illustrates the use of a deflecting means 14 which comprises av-shaped prismatic groove in wall 11 where both faces 26 and 27 of thegroove are made reflective and configured to redirect and couple thefocused light into waveguide 4 thus forming a bifacial prismatic groovedfeature. Ray R₁ enters face 26 making angle θ₁ with respect to surfacenormal to wall 10. Face 26 redirects ray R₁ so that it makes angle θ₂with respect to the same surface normal. Ray R₂ enters face 27 makingangle θ₄ with a surface normal to wall 10. Face 27 redirects ray R₂ sothat it makes angle θ₅ with respect to the same surface normaldirection. The slopes of faces 26 and 27 are selected to result in bothangles θ₂ and θ₅ being greater than θ_(C), which leads to trapping thelight in waveguide 4 and collecting the light at a terminal face of thewaveguide with concentration. Furthermore, prismatic grooves 14 can haveany other desired geometry and any desired number of faces that canreflect, refract, scatter or otherwise redirect light propagating withinwaveguide 4 so that the redirected light can be extracted from thewaveguide.

FIG. 10D illustrates the use of several smaller v-shaped prismaticgrooves being used instead of a single prismatic groove 14. It will berecognized that the plurality of reflective groove faces 26 are inclinedin accordance with the above principles to allow for efficient lightcollection in waveguide 4.

FIG. 10E illustrates a deflecting means 14 comprising one or morediffraction gratings. This grating may be implemented by way of exampleand not limitation, in the form of a hologram which is capable ofdeflecting the incident light at a suitable angle of TIR with respect towalls 10 and 11. The hologram can be formed in a glass plate or highlytransparent plastic film and can be made angularly and/or spectrallymultiplexed.

The foregoing embodiments of the present invention are described uponthe case where deflecting means 14 are of a reflective type. However,this invention is not limited to this and can be applied to the casewhen light deflecting means 14 is of a refractive type and the lightpasses through a portion of light deflecting means 14 rather than beingreflected from it. One such example is deflecting means 14 comprising aprism with a different refractive index embedded into waveguide 4 orattached to either its walls 10 or 11.

Furthermore, one or more embodiments of system 2 within the presentinvention can be configured to collect light rays in a preselectedspectral domain and/or only those rays that are propagating in waveguide4 in a predetermined range of acceptance angles. For example, thedeflecting means may comprise a reflective or transmissive hologramdesigned to deflect only a specific wavelength or a relatively narrowrange of wavelengths into waveguide 4 while allowing the otherwavelengths to pass without deflection.

Alternatively, in at least one embodiment of the invention, deflectingmeans 14 can comprise one or more layers of a dichroic material whichcauses the incident light to be split up into distinct beams ofdifferent wavelengths and allows only selected beam(s) to be trapped inwaveguide 4 while rejecting the rest of the spectral energy. In afurther example, light deflecting means 14 can be designed so that anyrays impinging onto its active aperture within an acceptance angle of upto a pre-determined value (e.g., up to 30 degrees) will be trapped inwaveguide 4. The remainder of the rays are deflected at angles smallerthe TIR angle θ_(C) with respect to surface normal direction 15 andthese latter rays can therefore be allowed to escape from waveguide 4.According to the above deflective means a combination or reflection andrefraction is provided which efficiently redirects light focused by therespective focusing means 6.

FIG. 11 illustrates an example of a waveguide structure according to thepresent invention which incorporates a deflecting means 14, which inthis example is implemented as a grooved structure formed in wall 10.Ray R₁ directed by focusing means 6 (not shown) enters waveguide 4 andstrikes deflecting means 14 at angle θ₁ with respect to a surface normaldirection 15 to wall 10. Deflecting means 14 deflects segment 17 of rayR₁ into segment 18 which propagates in waveguide 4 and forms angle θ₂with respect to surface normal direction 15 to wall 10. In the figurelight deflecting means 14 is configured with both a reflective face 26and a transparent face 55. Ray R₁ is reflected by face 26 and passesthrough face 55 into waveguide 4. Face 26 is inclined with respect towall 10 so as to result in angle θ₂ being greater than the TIR angleθ_(C). Similar to the embodiments described above, ray R₁ is thustrapped in waveguide 4 and will propagate through it by means of TIRfrom its longitudinal walls. Face 55 can be made approximatelyperpendicular to wall 10 or it can be inclined at any suitable anglewith respect to wall 10 or surface normal direction 15 so as to providean efficient light deflection into, and trapping within waveguide 4. Itwill be appreciated by those skilled in the art, that if segment 17 ofray R₁ lies in waveguide 4 (e.g., FIG. 6 through FIG. 8) angle θ₁ willgenerally be smaller than the TIR angle θ_(C) to provide for theentrance of R₁ from the lower refractive index medium of the outsidemedia into the higher refractive index medium of waveguide 4. Therefore,angle θ₁ will generally be smaller than angle θ₂ for the casesillustrated in FIG. 6 through FIG. 8. However, if segment 17 of ray R₁propagates outside waveguide 4 angle θ₁ can be of any suitable value andcan even be equal or exceed θ₂ provided that θ₂ is still greater thanthe TIR angle θ_(C).

FIG. 12 illustrates an example of the invention in which the collectorand waveguide are not separated by an air medium. In this example acladding or buffer layer 19 of optically transmissive material having arefractive index lower than that of waveguide 4. Layer 19 is separatingwaveguide 4 from collector array 5 providing for a stepped drop inrefractive index outwardly from waveguide 4 so that light can beinjected and trapped in waveguide and that system 2 has the same basicoperation as discussed above. Layer 19 can be positioned betweencollector array 5 and waveguide 4 so that system 2 forms a monolithicsandwiched structure. Suitable materials for layer 19 can include butare not limited to low refractive index monomers, polymers,fluoropolymers, low-n optical adhesives, thin films, materials commonlyused for cladding in optical waveguides or any other optically clearmaterial provided that its refractive index is lower than the refractiveindex of the material selected for waveguide 4. Particularly, amorphousfluoropolymers conventionally used for cladding optical waveguides suchas PFTE AF 1600 and PFTE AF 2400 can be utilized.

Additionally, wall 11 of waveguide is shown optionally provided with acladding layer 20 which also has a low refractive index so thatwaveguide 4 is encapsulated and protected from the outside media by alow-n material similar to conventional light guides. This can help avoidlight spillage from waveguide 4 toward improving the efficiency ofsystem 2. Cladding materials suitable for layer 20 can include any ofthe low-n materials mentioned above for layer 19. Alternatively, layer20 can be formed by a plastic reflective film or by metallization ofwall 11 to improve reflectivity or reduce light spillage through wall11. Another example of a suitable protective backsheet material forlayer 20 can be Polyvinyl fluoride (PVF), a fluoropolymer which iscommercially available as a film from DuPont and is sold under theTedlar® brand.

Similarly, any or all side walls 40 and 41 or end walls 35 and 36 ofwaveguide 4 can be encapsulated or otherwise covered by a protective orreflective layer and allowed to reflect light propagating in waveguide 4back into the waveguide by means of TIR or specular reflection. It willbe appreciated that layer 20 or encapsulation layers of any of thetransversal ends of waveguide 4 do not have to be optically transparentand can include opaque, light scattering or reflective materials. Yetfurther, system 2 can incorporate any other suitable layers, such asreflective or anti-reflective coatings, diffusers, radiation protectivecoatings or films, scratch and stain resistant coatings, light filteringfilms and the like. By way of example, waveguide 4, collector array 5 orany of their portions can be coated by dip coating, spin coating, vacuummetallization, applying a thin film using low-n adhesives, and so forth.Embodiments of the collector device discussed above can further compriseone or more light sources and/or light detectors or energy converters.

FIG. 13 illustrates an example embodiment in which a photoresponsiveelement, exemplified by photovoltaic cell 45, is disposed on wall 35. Byway of example, the photoresponsive elements can be attached to wall 35using an optical glue or transparent encapsulant, which preferably has athermal expansion coefficient and refractive index matching those ofwaveguide 4. A suitable buffer layer 19 based on a low-n fluoropolymerfilm is laid between collector array 5 and waveguide 4, thus forming amonolithic solid-state solar energy conversion device.

In FIG. 13, the ambient sunlight is collected from a large area ofcollector array 5 and brought to a much smaller area of face 35 ofwaveguide 4 thus causing a substantial concentration of solar radiation.It follows that system 2 of FIG. 13 can utilize a substantially smallerarea of raw photovoltaic materials than a conventional PV panel of asimilar power output and does not have the bulkiness and complexity ofconventional photovoltaic concentrators. A suitable heat sink (notshown) can be attached to the back of cell 45 to provide for efficientheat dissipation and reducing the operating temperatures of the cell. Anumber of such devices can be arranged in an array on a single metalsheet or frame and connected in series and/or in parallel to build thedesired power capacity.

Referring further to FIG. 13, the light deflected by deflecting means 14will undergo multiple reflections from at least walls 10 and 11.Additionally, some rays may undergo one or more total internalreflections from the side walls of waveguide 4. It will be appreciatedby those skilled in the optical arts that, as a result of the above, thelight rays will arrive at wall 35 from random directions and will strikethe surface of end wall (terminal wall) 35 at randomly distributedpoints. In other words, waveguide 4 will also act as a homogenizer ofthe concentrated light. Therefore, the concentrated light illuminatingcell 45 will have a more uniform energy distribution across the cellcompared to a case when the light is concentrated using a conventionaloptical device such as a lens or mirror which are generallycharacterized by highly non-uniform concentrated fluxes andsubstantially elevated peak flux densities in the center of the focalplane. It will also be appreciated that flux homogenization can befurther improved by increasing the number of deflecting means 14 and byincreasing the number of ray bounces from walls 10 and 11 which, inturn, can be for example accomplished by reducing the thickness ofwaveguide 4. However, the invention is not limited to the above but canalso be applied to the case when collecting means 6 and/or deflectingmeans 14 are positioned and aligned in accordance to a pre-selectedordered or randomized pattern. Alternatively, or in addition to, theside walls can be disposed at an angle with respect to each other toprovide for additional concentration or homogenization. Yet further, anyor all of the end walls 35, 36, or side walls 40, 41 can be curved orpatterned to direct the light propagating in waveguide 4 moreefficiently toward a pre-determined direction or a plurality ofdirections.

The foregoing embodiments are described upon the case where deflectingmeans 14 are arranged to trap incident light in waveguide 4 and directthe light in waveguide 4 toward a terminal end of the waveguide or wallsby means of at least TIR. However, this invention is not limited to thisbut can be applied to the case where deflecting means 14 are configuredto direct the light trapped in waveguide 4 toward a differentpre-determined area within the waveguide.

FIG. 14 illustrates an embodiment in which the matching pairs offocusing means 6 and deflecting means 14 are disposed symmetricallyabout a central line of symmetry of system 2 and configured to trap theincident light in waveguide 4 and direct the light toward a centralportion of the waveguide. One or more photoresponsive elements aredisposed on the device, for example a photovoltaic cell 45 attached towall 11 in close proximity to that central portion of waveguide 4 and isdisposed in energy receiving relationship from waveguide 4 to providefor the removal of light from the waveguide and collecting light by cell45. If wall 11 has a reflective or protective coating, such coatingshould have an opening in the area where cell 45 is attached.

By way of example and not limitation the photoresponsive element can becoupled to the waveguide element by a thin layer of optical adhesive ora photovoltaic encapsulant, such as silicone, EVA resin, or the like canbe provided between waveguide 4 and photovoltaic cell 45 to promoteadhesion and optical contact between cell 45 and waveguide 4. Forefficient light removal, the refractive index of the adhesive orencapsulant should preferably be close to or greater than the refractiveindex of the material of waveguide 4. This matching of refractiveindices will ensure that no TIR occurs in the area where cell 45 isattached to wall 11 and the light striking that area is allowed toescape from waveguide 4 and enter into cell 45.

Referring again to FIG. 14, this embodiment can be arranged to have alinear configuration with a plane of symmetry perpendicular to thedrawing plane, similar to that of FIG. 12, in which case collector array5 can be formed by a lenticular lens array and the matching array ofdeflecting means 14 can be formed by parallel prismatic grooves made inwall 11.

FIG. 15A-15D illustrates example embodiments of collector arrays withdifferent rectangular or circular arrangements, each being shown withexample rays striking the collector and being directed inwardly to thelight harvesting area. In FIG. 15A collector array 5 and waveguide 4 isshown with a planar shape having a square or rectangular outline. Alight harvesting area 47 (indicated by a hatched area) is configured,such as with a rectangular shape and surface area substantially smallerthan the surface area of collector array 5 and/or waveguide 4 in orderto obtain sufficient light concentration.

FIG. 15B illustrates an embodiment with an axial symmetry in which casecollecting means 6 and deflecting means 14 have an annular configurationformed by a revolution of the cross sectional design shown in FIG. 14around an axis of symmetry by a full or partial angular turn. In such anaxisymmetrical configuration, the collector array 5 and waveguide 4 havea round outline.

FIG. 15C illustrates an embodiment similar to that of FIG. 15B, but cutwith a rectangular or square outline, or to any other desired shape oroutline (e.g., hexagonal, sectorial, and so forth), depending on theapplication, packing requirements, aesthetics and/or desired operatingparameters. Harvesting area 47 can have a round shape as shown in FIG.15B and FIG. 15C or it can be of any other suitable shape. Harvestingarea 47 can be formed on either wall 10 or 11 where it can be centrallylocated or offset relative to the center forming an asymmetricconfiguration.

FIG. 15D illustrates an embodiment in which the harvesting area 47 isconfigured on or at any of the terminal ends of waveguide 4. The figureshows a device in which collector array 5 is based on annular lenticularlenses focusing incident light onto a plurality of deflecting means 14underneath (not shown) which are following the circular pattern offocusing means 6. This configuration allows for forming a point-likeharvesting area 47 at wall 35 of waveguide 4. It should also beunderstood that system 2 can be configured to have multiple harvestingareas as desired. Further, waveguide 4 may be tapered such that anoverall length or width of waveguide 4 is reduced or enlarged asdesired.

FIG. 16A and FIG. 16B illustrate different perspective views of system 2in an exemplary annular configuration where light harvesting area 47 islocated in the central portion of such an axisymmetrical, collectiondevice. While a full-circle round configuration of system 2 is shown inthe figures, it should be appreciated that the collector can be laid outin any desired shape or layout, either symmetric or asymmetric, or maycomprise any desired portion of the illustrated annular configuration.

Yet further, although the foregoing embodiments of system 2 arediscussing a planar configuration, the invention is not limited toplanar light collection devices. It can also be applied to a case whencollector array 5 and waveguide 4 are made of a flexible material whichis configured for bending and can be shaped, for example, in acylindrical configuration. It will be appreciated, however, that inresponse to an excessively tight bend radius, for a given thickness ofwaveguide, that the internal light reflections can reach below thecritical angle required to achieve total internal reflections, thusleading to a loss of light.

FIG. 17 through FIG. 19 illustrate point focus lens collectorembodiments by way of example and not limitation. Although, thepreceding embodiments described collector means which were organized inlinear or lenticular configurations, the present invention can beimplemented in a wide range of point focus configurations. In FIG. 17illustrates collector array 5 formed by a planar lens array wherecollecting means 6 has a configuration of point-focus lenses having around shape, positioned adjacent to each other and arranged in a regulargeometric pattern, shown depicted for the sake of simplicity with rowsand columns on a single transparent substrate.

In FIG. 18 the packing factor of the lenses is increased in response toeliminating the non-lens areas and overlaying small external portions ofeach lens. It should be understood that a packing factor of up to 100%can be achieved, for example, by using square-shaped or hexagonallenses. Square-shaped lenses are shown in FIG. 18 which completely fillsthe receiving surface of collector array 5 with point-focus lenses.Collecting means 6 is shown implemented in a tight square pattern whichmore efficiently covers the surface area of collector array 5.

In FIG. 19 a hexagonal arrangement of collecting means 6 is shown inwhich point-focus lenses form a planar array with about 100% packingfactor. Suitable arrangements of point-focus collecting means 6 mayinclude other placement patterns and spacing between individualelements.

FIG. 20 illustrates a waveguide embodiment configured with deflectingmeans configured for point focus collection, such as depicted in FIGS.17-19. When using a point focus collecting means, it will be appreciatedthat the deflecting means may still comprise an elongated deflectingmeans 14, such as shown in FIGS. 4A-4B and FIG. 12, to receive focusedbeams from multiple focusing means 6 and inject the beams into waveguideat TIR angles with respect to at least walls 10 and 11. However, for thereasons of minimizing the interference with the light propagating inwaveguide 4, as discussed above, the prismatic grooves can be separatedinto point focus deflectors which are each substantially smaller inwidth in the longitudinal direction to take advantage of the smallersize of the focal area in a point focus collector configuration versusthe linear focus. By way of example, the base of a prismatic groove madein wall 11 can have a square shape dimensioned to closely approximatethe focal area of the respective point-focus focusing means 6 as seen inFIG. 20. In response to the use of separate point-focus deflectors,deflecting means 14 will occupy much less volume of waveguide 4 and takemuch less space from wall 11 thus reducing the chance of interceptinguseful light propagating in waveguide 4. FIG. 20 shows an arrangement ofdeflecting means 14 formed by small-area square-shaped prismatic groovesin wall 11 of waveguide 4.

By way of example and not limitation, each of the separate deflectiongrooves shown in FIG. 20 has a triangular or v-shaped cross section in aplane parallel to side wall 40 so that each groove forms at least onereflective face 26 to trap incident light in waveguide 4. In the figure,the combined area of deflecting means 14 when projected to a planeperpendicular to the prevailing direction of light propagation inwaveguide 4, will be reduced compared to a case when linear grovesextend all the way from wall 40 to the opposing side wall and can bemade much smaller than the cross section of waveguide 4 in the sameplane. Therefore, the interference of deflecting means 14 with the lighttrapped in waveguide 4 will generally be less in a point focusconfiguration of both focusing means 6 and deflecting means 14 incomparison to a linear focus design.

The foregoing embodiments are described upon the case when collectorarray 5 is of a refractive type. However, this invention is not limitedto this but can also be applied to the case when collector array 5 is ofa reflective type. By way of example, collector array 5 can be formed bya dense planar array of micro-mirrors in which case each focusing means6 can be represented by a concave reflector which has a mirrored surfaceand is configured to focus an incident beam of light onto a respectivedeflecting means 14. Each mirror can have a spherical shape, parabolicshape or any other shape resulting in collection of the incident lightto a substantially smaller area than the aperture area of the mirror. Inanother example, each mirror in collector array 5 can be formed by amicro-array of planar reflectors inclined at suitable angles, such as aFresnel mirror, so as to result in efficient focusing of the incidentradiation.

FIG. 21 illustrates a collector device embodiment 2 which comprises acollector array 5 having a planar transparent body upon whose surface isdisposed a densely packed array of micro-mirrors. Thus, each collectingmeans 6 is formed by a micro-mirror which is integral to the planartransparent body. Each micro-mirror has a curved mirrored surface thatallows it to efficiently collect incident light and focus the light ontoa corresponding deflecting means 14 having a substantially smalleraperture. Similarly to lenses in a lens array, micro-mirrors can bedesigned in linear or point focus configurations. Waveguide 4 isconfigured in the form of a planar transparent plate whose refractiveindex is greater than that of the outside media. In similar manner asthe examples discussed above, each deflecting means 14 can comprise aprismatic grooved feature in wall 11 having reflective face 26 and whichis optically coupled to waveguide 4. Both parallel walls 10 and 11 ofwaveguide 4 are also made transparent to the incident light.

In operation, incident ray R₁ enters waveguide 4 first, and passesthrough the waveguide into collector array 5. Ray R₁ is further focusedby the mirror surface of an individual focusing means 6 and is directedto the face 26 of a prismatic groove of a respective deflecting means14. Face 26 is inclined with respect to a surface normal direction towalls 10 and 11 and it redirects ray R₁ into waveguide 4 at an anglewith respect to a normal to walls 10 and 11 greater than critical angleθ_(C), so that ray R₁ further propagates in waveguide 4 by means of atleast TIR toward terminal end 35. Accordingly, rays R₂, R′₁ and R′₂ arealso injected into waveguide 4, trapped in waveguide 4 by means of TIRand directed generally toward the same direction. Similarly to the lightcollection system of FIG. 12, a transparent cladding or buffer layermade of low-n material can be laid between collector array and waveguide4. Further, a cladding and/or protective layer or layers can be added towall 11 and/or side walls of waveguide 4 to protect it from theenvironment. Further details of operation of system 2 shown in FIG. 21as well as its possible variations configurations will be apparent fromthe foregoing description of preferred and other embodiments.

FIG. 22 illustrates an example embodiment which does not include thecladding material between the collector and the waveguide. The precedingembodiments have been described comprising a space or a cladding layerbetween collector array 5 and waveguide 4 which has a suitable opticalinterface 8 for trapping light in waveguide 4 formed by the interfacebetween waveguide 4 and that space or cladding layer. However, it shouldbe appreciated that embodiments of the present invention are not limitedto the use of this cladding space. Alternatively, as exemplified in FIG.22, the stepped drop in refractive index outwardly from waveguide 4 canalso be created by providing a smaller refractive index for collectorarray 5 compared to that of waveguide 4.

In FIG. 22 is depicted a cross section of a waveguide 4 in which arefractive index n₁, collector array 5 has a refractive index n₂ withn₁>n₂. More particularly, collector array 5 is configured with a lowerrefractive index n₂ than waveguide 4 and can be disposed thereon (e.g.,molded directly on waveguide 4 or otherwise attached to wall 10), sothat the line of its attachment to the waveguide forms interface 8 whichallows rays to enter into waveguide through wall 10 but reflectsoutgoing rays that have an incidence angle greater than critical angleθ_(C). By way of example, a high refractive index glass, such as LASF35glass manufactured by Schott and having the refractive index n₁ ofaround 2, can be used for waveguide 4 while PMMA with refractive indexn₂ of around 1.49 can be used to create such interface 8 at wall 10 ofthe waveguide. As with the examples described above, each lightdeflecting means 14 redirects light incident from the respectivefocusing means 6 at an angle greater than a critical angle of TIR, whichis in this case is about 48.16° that results in trapping the light inwaveguide 4 and concentrating the light at wall 35.

The present invention is also not limited to the case when collectorarray 5 and waveguide 4 are disposed in a stationary position withrespect to each other and can also be applied to the case when collectorarray 5 and waveguide 4 can be disposed in any one of a translated, areversed, and/or a rotated orientation relative to each other towardachieving different light concentration or altering the acceptanceangle. Furthermore, collector array 5 and waveguide 4 can be mademovable with respect to each other to provide for fine tuning theacceptance angle or for tracking the source of light.

2. Illuminator Embodiments

The present invention teaches both optical collector embodiments asdescribed above, and optical illumination devices which are discussedbelow.

FIG. 23A and FIG. 23B illustrate example embodiments of an illuminationdevice. Referring to FIG. 23A, optical illumination device 2 is shown byway of example comprising a optically transparent multimode planarwaveguide 4 and a light collimating array 5, such as a planar lenticularlens array, disposed adjacent to waveguide 4 so that waveguide 4 andlens array 5 form a planar sandwich-like configuration. FIG. 23Bprovides a better view of the waveguide portion of the device shown inFIG. 23A. It should be appreciated that although the planar waveguide isoptically transparent, it can be subject to optically losses and needonly be sufficiently optically transmissive for the given application towhich it is directed.

Referring to FIG. 23A and FIG. 23B, waveguide 4 is formed by anoptically transmissive body having a general appearance of a rectangulartransparent plate or a slab. Waveguide 4 is configured to have opposinglight transmissive faces 10 and 11 extending parallel to a predominantplane 9, a side face 40 and an opposing side face 41 generallyperpendicular to faces 10 and 11, as well as opposing terminal faces 35and 36 each being generally perpendicular to faces 10, 11, 40 and 41.The thickness of waveguide 4 is selected to be substantially less thanthe planar dimensions (length and width) of the waveguide 4 so that thesurface area of either planar face 10 or 11 is substantially larger(e.g., preferably one or more orders of magnitude) than the area of atleast one of the terminal faces 35 and 36. Furthermore, waveguide 4 isconfigured to transmit light by means of a total internal reflection(TIR) along at least its light conducting faces 10 and 11 and generallytoward at least one of the terminal faces 35 and 36. By way of example,waveguide 4 can be configured so that a light ray entering waveguide 4through its face 35 can be guided generally in one direction toward theopposing face 36 by means of light conduction through the body ofwaveguide and by means of bouncing the light from faces 10 and 11 due toTIR.

If used at optical frequencies, waveguide 4 can be made from any highlytransparent material such as glass, PMMA or polycarbonate. Othertransparent materials or substances, such as a liquid or a siliconrubber can also be used for making at least a portion of the body ofwaveguide 4. In order to enhance its optical guiding ability, thematerial of waveguide 4 can have a relatively high index of refraction,and can be surrounded by a material with lower refractive index. In sucha case, the structure can guide optical waves by means of TIR and can becharacterized by a critical angle θ_(C) so that when a ray of lightpropagating within waveguide 4 strikes a waveguide boundary at an anglelarger than θ_(C) with respect to the normal to the boundary surface,the ray is reflected back into waveguide 4. Faces 10 and 11 shouldnormally be smooth or polished so as to avoid or minimize parasiticlight scattering when undergoing TIR reflections from the faces. Whenappropriate, face 11 can be configured with a mirrored surface toenhance light guiding properties of waveguide 4.

Additionally, side edges of waveguide 4 (faces 40 and 41 in FIG. 23A andFIG. 23B) can be configured as smooth surfaces capable of reflect lightby means of TIR or specular reflection so that the light is kept in thewaveguide even when it reaches either of the side edges of waveguide 4.Metallization, a reflective film or other type of mirror finish can beapplied to either one or both faces 40 and 41 to further enhancereflectivity and the ability of the waveguide to conduct light. Face 36can also be made specularly reflective in order to reflect any lightarriving at it from the inside of waveguide 4 back into the waveguidethus effectively reversing the path of the light back toward face 35.

In accordance with a preferred embodiment, waveguide 4 comprises aplurality of light deflecting elements optically coupled to waveguide 4.The term “optically coupled” is meant herein to describe anyrelationship between a first optical component and a second opticalcomponent which enables light to pass from the first optical componentto the second optical component. Reference to optically coupled does notpreclude various forms of optical losses. Also, it should be appreciatedthat this term also includes implementations in which the first andsecond optical components are separated by one or more opticalinterfaces or layers at which the light may undergo respective opticallosses (e.g., parasitic reflections, Fresnel reflections, attenuation,and so forth) and/or changing of its direction of propagation (e.g.,refraction at the interface between two media having differentrefractive indexes). For the purpose of demonstrating a preferred modeof the present invention, the light deflecting elements are representedby surface relief features associated with face 11, more specifically,parallel v-shaped prismatic grooves 14 made in face 11, as shown in FIG.23A and FIG. 23B.

As previously described, prismatic grooves 14 can be produced by any ofa variety of known methods of creating surface relief such asmicro-structures and/or texture. These structures can be fabricatedusing a technique for direct material removal including mechanicalscribing, laser scribing, micromachining, etching, grinding, embossing,imprinting from a master mold, photolithography, other known mechanisms,and combinations thereof. If required, the faces of prismatic grooves 14can be further polished to obtain a very smooth surface. It will beappreciated that waveguide 4 can also be made with grooves alreadyembedded into it by means of casting, injection molding, compressionmolding or the like processes, such as might arise in a mass productionenvironment.

Alternatively, waveguide 4 can incorporate a layer of transparentmaterial, such as a plastic film or thin transparent plate, attached toface 11 and the prismatic grooves 14 can be formed in that layer.Optical lithography can be used to create the required pattern in alight-sensitive chemical photo resist by exposing it to light (typicallyUV) either using a projected image or an optical mask with a subsequentselective removal step of unexposed parts of a thin film or the bulk ofa substrate.

In another alternative, the transparent material can be overmolded ontowaveguide 4 in the respective areas and prismatic grooves 14 can beformed in the overmold. A negative replica of prismatic grooves 14 canbe made by diamond cutting/machining, laser micromachining, ion beametching, chemical etching, or any similar material removal techniquefollowed by imprinting in an overmold process. In the illustrated case,prismatic groves 14 or tapered prismatic voids in face 11 extendend-to-end from face 40 to face 41 and are optically coupled towaveguide 4 directly through the surface of waveguide 4, preferablywithout the use of additional optical interfaces or layers which aresubject to associated losses.

Referring again to FIG. 23A and FIG. 23B, lens array 5 is formed by anoptically transmissive body having a generally planar rectangular shapewith the length and width dimensions approximating those of waveguide 4.Lens array 5 is configured to have a planar face 12 facing waveguide 4and forming an entrance aperture and an opposing face 16 forming an exitaperture. Further, lens array 5 comprises a plurality of cylindricallinear lenses 6 (also referenced heretofore to as lenslets) associatedwith face 16 and arranged on a single substrate in a planar array. Theindividual lenslets of lens array 5 are made an integral part of thebody of lens array 5 and positioned adjacent to each other with a highpacking factor to form a generally planar, three dimensionally texturedsurface. Lenses 6 forming planar lens array 5 can be lenticular,linear-focus, or point-focus and can be packed with any desired densitycovering the entrance aperture of lens array 5. The lens array can befabricated using any conventional method such as replication, molding,micromachining, chemical etching, beam etching and the like. Theindividual lenses can be made an integral part of collector array 5 andmade from the same material as that of the body of the array.Alternatively, the lens array can be formed on a transparent substrateplate and can be made either from the same or a different material thanthe substrate plate. Individual lenses can also be made as separatepieces and attached to the substrate plate. The placement of lenses inthe lens array can be arranged according to any desired pattern, insofaras the light is collected on the deflection elements within thewaveguide. For example, the lenses can be spaced apart, contacting eachother or overlapping and can be positioned in any desired pattern in theplanar array.

Lens array 5 is positioned in a close proximity and generally parallelto waveguide 4 and disposed in an energy receiving relationship withrespect to waveguide 4. Energy receiving relationship is meant to meanany relationship between waveguide 4 and collector array 5 which enableslight exiting waveguide 4 to enter into the collector array. Accordingto a preferred embodiment, collector array 5 is positioned to receivelight emerging from waveguide 4 through its face 10. For this purpose,lens array 5 is aligned with respect to waveguide 4 so that its face 12is disposed in a close proximity and parallel to face 10 of waveguide 4forming a sandwich structure. Face 12 of lens array 5 is configured totransmit a substantial portion of light emerging from face 10 ofwaveguide 4 into lens array 5.

The number and placement of individual lenslets in lens array 5 areselected so that each lens 6 corresponds to a prismatic groove 14,extends parallel to the prismatic groove 14 and is aligned with respectto the prismatic groove 14 along a perpendicular to face 10 of waveguide4.

Each prismatic groove 14 is configured to intercept a portion of thelight beam propagating through waveguide 4 by its active area (alsoreferenced heretofore as an entrance aperture of prismatic groove 14)and redirect the portion of the light beam toward face 10 of waveguide 4and at a greater angle with respect to face 10 so that the condition ofTIR is not met for the redirected light and it can exit from waveguide 4and subsequently enter lens array 5.

Each lenslet in lens array 5 is configured to receive a divergent beamof decoupled light emerging from waveguide 4 after being redirected by amatching prismatic groove 14 and collimate the divergent beam into aquasi-parallel beam propagating perpendicular to plane 9 and away fromoptical device 2.

Naturally, one of the best modes illustrating the present invention mayemploy such an arrangement of optical device 2 in which each prismaticgroove 14 is disposed at or near the focus of the respective lens 6 andthe receiving aperture of prismatic groove 14 is substantially smallerthan the entrance aperture of the respective lenslet 6. Prismaticgrooves 14 can be made sufficiently spaced apart from the respectivelenses 6 to allow for efficient light collimation. For the purpose ofthis invention and from the practical standpoint, the terms “focal area”or “focus” of lens 6 should be understood broadly and generally refersto a relatively small area within the envelope of a focused beam thatthe lens 6 would have produced if illuminated by a generally parallelinput beam of light. The focal area generally has a cross sectionsubstantially smaller than the cross section of respective lens 6.Accordingly, the focal area can also include areas at a relatively smalldistance from the “ideal” focus of lens 6 and also where the focusedbeam can be convergent (before focus) or divergent (after focus).

In accordance with this invention, it is preferred that an effectivefocal length of each lens 6 is substantially shorter than the dimensionsof faces 10 and 11 in order to achieve better compactness of device 2.For the purpose of this invention, the term “effective focal length”generally refers to the distance between lens 6 and its focus. This termshould also be understood broadly and it also includes the cases whenthe focal length of the same lens 6 can change depending on the opticalproperties of the material filling up the space between lens 6 and thefocus. Accordingly, the location of the effective focal area, and thusfocal length, may be different if a different material separates lens 6and its focal area. By way of example, for the same parameters of lens6, its focal distance can be longer in PMMA material than in the air dueto the difference in refractive indexes.

In accordance with preferred embodiments, waveguide 4 should beoptically separated from lens array 5 by at least one optical interfacethat allows for propagating the light in waveguide 4 by means of TIRwithout escaping into array 5. A suitable optical interface 8 can becreated by various means. For example, interface 8 can be a physicalboundary or wall of the body of waveguide 4 which is surrounded byoutside media with lower refractive medium, such as air. Alternatively,it may comprise an interface between two media having differentrefractive indices so that the refractive index decreases along theoptical path from waveguide 4 toward lens array 5. By way of example andnot limitation, an interface of this type can be obtained by separatingwaveguide 4 from the body of lens array 5 (or from bodies of individuallenses 6) by introduction of a thin layer of air, lower refractive indexmaterial, or any other boundary between higher and a lower refractiveindex material. In a more specific example, interface 8 can comprise aninterface between glass, PMMA or polycarbonate (high refractive index)and a low refractive index polymer or air. By way of example, waveguide4 can be partially or entirely surrounded by ambient air. Alternatively,a layer of cladding material can be provided between waveguide 4 andlens array 5 in which case, the optical device can form a monolithicsystem while maintaining the same basic structure and operation. In atleast one preferred embodiment of the present invention, waveguide 4spaced apart from lens array 5 so that a layer of ambient air isdisposed therebetween with interface 8 formed by face 10 being theboundary between waveguide 4 and layer of ambient air.

In operation, the optical device illuminator can be better understoodfrom a cross sectional schematic representation of the device and itscomponents, as well as from analyzing the paths of individual light raysin the device.

First, turning to the prior art, FIG. 24 and FIG. 25 illustrate theoperation of conventional collimating systems typically employing alarge-aperture optical collimating device such as lens 75 (FIG. 24) ormirror 85 (FIG. 25). Rays 180 and 181 emanating from a light source 145are being collected by the receiving aperture of the collimators anddirected/collimated in a direction parallel to the optical axis andperpendicular to the focal plane of lens 75 or mirror 85. Each lens 75and mirror 85 can be characterized by a transversal size D and a focallength F. In the prior art, an uncollimated light source 145 is usuallyplaced in the focus of the lens or mirror at a considerable distancefrom the collimating device. Also, it will be appreciated by thoseskilled in the art that, when light source 145 has a finite transversalsize D_(S), in order to obtain useful collimation of the light, thecollimator's size D should be significant larger than D_(S) as a matterof optics. These aspects of the conventional design result in overallsize and weight increases which limit applicability.

In comparison to the above, an embodiment of optical device 2 as FIG.23A is configured so that a ray 130 enters waveguide 4 from its edge andis propagated through waveguide 4 by TIR until it strikes one of theprismatic grooves 14 which deflect ray 130 out of the waveguide andtoward lens array 5. A lenslet 6 further collects ray 130 and collimatesit into a direction generally perpendicular to plane 9. Further detailsof the operation of device 2 and the path of ray 130 illustrated in FIG.23A will be apparent from FIG. 4A and its description considering thereversing of ray 30.

FIG. 26 illustrates an example illuminator embodiment 2 shown configuredfor collimating otherwise uncollimated light emanated by light source145 in a more space efficient manner. Source 145 is positioned so thatit illuminates an edge of waveguide 4, the edge represented by face 35,allowing the light to enter waveguide 4 and propagate in the waveguidegenerally toward the opposing face 36 while being confined between faces10 and 11 due to TIR. Light source 145 can be of any known type,including but not limited to incandescent lighting, heat emittingbodies, light emitting diodes (LEDs), lasers, sunlight, light/heatscattering, radiating surfaces, or any other devices or combinationsthereof adapted for generating light. The shape of the incident beam maybe optionally formed by any desired optical system which provides asuitable angular and/or spatial energy distribution in the beamilluminating the side edge of waveguide 4. For example, a lightcollimating device can be used to produce a beam of light with asuitable angular spread. In another example, one or more optical fiberscan be used to deliver and input light into waveguide 4 through face 35.

In at least one preferred implementation of FIG. 26, waveguide 4comprises a highly transparent material having a refractive index n₁which should be generally greater than a refractive index n₂ of theoutside medium (n₁>n₂). In an exemplary case of waveguide 4 being madefrom PMMA or glass, n₁ can be a value of about 1.5. In response to thepresence of a thin cushion space between collector array 5 and waveguide4, there is a layer of air whose refractive index is about 1, and whichadjoins face 10 of waveguide 4. Furthermore, since waveguide 4 issurrounded by air, the refractive index increases outwardly at eachexternal face of waveguide 4 including faces 10 and 11. Faces 10 and 11serve as TIR reflectors for light propagating in waveguide 4 at angleswith respect to a surface normal direction of faces 10 and 11 greaterthan θ_(C), which is a critical angle of TIR. Face 10 serves as opticalinterface 8 between waveguide 4 and lens array 5.

According to Snell's law of optics, when light passes through a boundarybetween a first refractive medium and a second refractive medium, n₁ sinϕ₁=n₂ sin ϕ₂, where n₁ and n₂ are the refractive index of the firstmedium and the second medium, respectively, with ϕ₁ and ϕ₂ being theangle of incidence and the angle of refraction, respectively.Furthermore, the critical angle of TIR θ_(C) is the value of ϕ₁ forwhich ϕ₂ equals 90°. Accordingly, θ_(C)=arcsin (n₂/n₁·sin ϕ₂)=arcsin(n₂/n₁), which makes θ_(C) approximately 42.155° for an exemplary caseof the interface between PMMA with the reflective index n₁ of about 1.49and air with n₂ of about 1.

Prismatic grooves 14 are formed in face 11 where the size of individualprismatic grooves 14 and their number are selected so that they can bespaced from each other by a distance which is generally substantiallylarger than the receiving aperture of each prismatic groove. Prismaticgrooves are shown as identical structures and approximately evenlyspaced along face 11 in FIG. 26. However, it should be appreciated thatthese structures can have different individual sizes, shapes, andspacing without departing from the teachings of the present invention.

Each prismatic groove 14 is configured to have a light receivingaperture comprising a sloped reflective face that is positioned tointercept a portion of the light propagating along waveguide 4 andredirect the portion of light toward face 10 at such an angle so as toresult in the portion of light passing through face 10 and into lensarray 5. This can be achieved by the following. At least one face ofeach prismatic groove 14 is made reflective. The face of prismaticgroove 14 is also exposed to the light propagating along waveguide 4 andpositioned at an angle with respect to the prevailing direction of thelight propagation in waveguide 4. As a result, the light incident ontothe exposed face of prismatic groove 14 is redirected from its originalpropagation path in waveguide 4 and is directed onto face 10 ofwaveguide 4 generally at an angle with respect to face 10 which exceedsthe TIR angle, thus allowing the redirected light to exit (decouple)from waveguide 4.

Upon exiting from waveguide 4, the redirected light enters lens array 5and is collected by lens 6 matching the respective prismatic groove 14.Since prismatic groove 14 is disposed at or near the focus of therespective lens 6 in a matching groove-lens pair, the light collected bylens 6 is collimated into a generally parallel beam propagating alongthe optical axis of lens 6. When each of the lenses 6 forming lens array5 has an optical axis perpendicular to the lens array 5 and the matchingprismatic groove 14 is disposed on the optical axis, lens array 5 willform an array of collimated beams propagating away from it andperpendicular to its surface. Thus, the optical illuminator devicereceives a generally uncollimated light incident on its side edge,distributes the light through the body of waveguide 4 and emits a highlycollimated parallel beam of light from the device's frontal surface.

More particularly, the operation of the optical illuminator device canbe illustrated by exemplifying the paths of individual light rays.Referring again to FIG. 26, a ray R₁₀₁ is seen emanating from lightsource 145 and entering waveguide 4 through face 35, at a skew anglewith respect to face 10, and which then strikes face 10. In response toan angle of incidence 121, with respect to the surface normal directionof face 10, which is greater than TIR angle θ_(C), ray R₁₀₁ is reflectedback into waveguide 4. Ray R₁₀₁ then approaches face 11 and strikes areflective face of prismatic groove 14 where it is redirected againtoward face 10 of waveguide 4 at an angle for which the condition of TIRis not met at the optical interface created by face 10 and the outsidemedia. Thus, prismatic groove 14 provides a deflection angle for rayR₁₀₁ to assure that R₁₀₁ is deflected to an angle of incidence 122 thatis smaller than θ_(C). In response to this angle of incidence,redirected ray R₁₀₁ has an angle which is now smaller than θ_(C),wherein ray R₁₀₁ exits from waveguide 4 through face 10 with some benddue to refraction, passes through a thin layer of lower refractive indexmedium and enters lens array 5 where it is intercepted by lens 5 anddirected away from optical device 2 in a direction generallyperpendicular to the prevailing plane 9 of optical device 2.

Similarly, a different ray R₁₀₂ emitted by source 145 and enteringwaveguide 4 at a skew angle with respect to waveguide faces 10 and 11propagates along waveguide 4 by bouncing from its faces until it strikesa different prismatic groove 14 at face 11. Ray R₁₀₂ is also redirectedback toward face 10 at an incidence angle which is smaller than θ_(C)that allows ray R₁₀₂ to decouple from waveguide 4 and enter therespective lens 6 which further collimates R₁₀₂ generally into the samedirection as ray R₁₀₁. It will be appreciated by those skilled in theart that additional rays randomly entering face 35 within apre-determined range of angles will be initially trapped in waveguide 4and propagated toward face 36, and then in response to striking aprismatic groove 14 the rays are deflected out of the waveguide andcollimated by the lens array 5.

FIG. 27 illustrates an embodiment of illumination device 2 having aplurality of lenses 6 which intercept and redirect the random raysemitted by source 145 and injected into waveguide 4 through face 35. Theredirected rays are decoupled from waveguide 4 and are furthercollimated by lens array 5 into a parallel beam. As the light passesthrough the illumination device it is deflected, distributed andcollimated prior to exiting lens array 5.

It should be understood that, while only few rays are shown in FIG. 27for the sake of illustrative clarity, the optical illumination devicecan operate with any number of rays within a predetermined acceptanceangle and in a desired spectral range of the incident light.Accordingly, prismatic grooves 14 can be configured to receive a fan ofrays having a predetermined angular spread and redirect the rays at asufficient bend angle so that at least a substantial portion of the raysis decoupled from waveguide 4 and is further collimated by lens array 5.It will be recognized, therefore, that if a moderately divergent beam ofmonochromatic or broad-spectrum electromagnetic energy enters planarwaveguide 4 through a small-area terminal end of the waveguide, thelight is distributed through the volume of the waveguide and exits ascollimated light (substantially parallel) across a substantially largersurface area.

Only four prismatic grooves 14 and four matching lenslets 6 are shown ineach of FIG. 26 and FIG. 27 for clarity. However, it should beunderstood that waveguide 4 and lens array 5 can incorporate anysuitable number of prismatic grooves 14 and lenses 6, respectively, toprovide for a desired operation and light extraction and collimation. Inorder to increase the decoupling efficiency of light propagating inwaveguide 4, the sizes and placements of individual prismatic groovescan be so selected and the longitudinal dimensions of waveguide 4 can beincreased to a point when practically all of the light rays incidentinto waveguide 4 through its face 35 have a chance of being decoupledand collimated, so that practically no optical energy is lost.

Additionally, it will be appreciated that face 36 can be mirrored and/orinclined at an angle with respect to face 10 so that the light raysreaching face 35 will be directed back into waveguide 4 as theirpropagation direction will be reversed which will increase the lightextraction/decoupling efficiency. For this purpose, the second face ofeach prismatic groove 14 can be made reflective and positioned at asuitable angle to intercept the reversed rays and decouple them in themanner described above. Also, as described above, various faces ofwaveguide 4 participating in TIR can be selectively mirrored and/orprovided with a cladding layer to promote reflection and protection ofthe device from the environment. Mirroring can be obtained by depositinga reflective layer using any known means, such as, for example utilizinga coating, such as silver, aluminum, or laminating with a reflectivefilm, or other known techniques and combinations for increasing theefficiency of light reflection.

The size of prismatic grooves 14 is exaggerated for clarity in theillustrations discussed above. However, it should be understood that theindividual grooves 14 should preferably be substantially smaller in sizethan the width of each respective lenslets 6 toward improvingcollimation efficiency. Furthermore, it should be understood that thedimensions of the prismatic grooves 14 is also exaggerated for claritywith respect to the dimensions of waveguide 4 as well, while a specificapplication may require a micro-scale size of prismatic grooves 14whereas lens array 5 may comprise a large number of micro-lenses whichcan be very small compared to the dimensions of the array.

FIG. 28 depicts a detailed ray tracing according to at least oneembodiment of the illumination device according to the presentinvention. Waveguide 4 is configured with a higher refractive index n₁than the surrounding medium (n₂) which permits propagation of a raydespite it being received at a relatively sharp angle with respect tothe prevailing material plane and surfaces 10 and 11. As shown in thefigure, a ray R₁₁₀ impinges onto face 35 of waveguide 4 at an incidenceangle θ_(in) with respect to a normal to face 35 and enters waveguide 4at a refraction angle θ_(r) with respect to a surface normal directionof face 35.

Ray R₁₁₀ can propagate in waveguide 4 when its refraction angle θ_(r)permits for TIR at faces 10 and 11. Therefore, a maximum refractionangle θ_(r max) can be defined as 90−θ_(C). From Snell's law theequation n sin θ_(in max)=n₁ sin θ_(r max), is obtained where n is therefractive index of the medium adjacent to face 35 of waveguide 4 andθ_(max) is a maximum incidence angle that waveguide 4 will accept. Sincesin θ_(r max)=sin (90°−θ_(C))=cos θ_(C), n sin θ_(in max)=n₁ cos θ_(C)is obtained which can be further transformed to the following.

${\frac{n^{2}}{n_{1}^{2}}\sin^{2}\theta_{{in}\mspace{11mu} \max}} = {\cos^{2}\theta_{C}}$

Furthermore, since

${{\cos^{2}\theta_{C}} = {{1 - {\sin^{2}\theta_{C}}} = {1 - \frac{n_{2}^{2}}{n_{1}^{2}}}}},$

obtain the following relationships:

${{\sin \; \theta_{r\mspace{14mu} \max}} = {{\frac{\sqrt{n_{1}^{2} - n_{2}^{2}}}{n_{1}}\mspace{14mu} {and}\mspace{14mu} n\mspace{11mu} \sin \; \theta_{{in}\mspace{11mu} \max}} = \sqrt{n_{1}^{2} - n_{2}^{2}}}},$

where the expression n sin θ_(in max) can be defined as a numericaperture NA of waveguide 4.

An imagery cone having an angular size of 2 θ_(in max) (±θ_(in max) froma normal to face 35 of waveguide 4) can be defined as an acceptance coneof waveguide 4 for the purpose of illustrating this invention and theangle 2 θ_(in max) can be referenced as an acceptance angle of waveguide4.

In FIG. 28, a case is illustrated when θ_(in)<θ_(in max) which resultsin θ_(r) being less than 90−θ_(C) and θ₁₀₁ being greater than TIR angleθ_(C). Subsequently, ray R₁₁₀ propagating in waveguide 4 strikes face 10at point P₁₀₁, where it makes angle θ₁₀₁ with a surface normal directionto parallel faces 10 and 11 and undergoes a practically lossless totalinternal reflection. Upon reflecting by means of TIR, ray R₁₁₀ isfurther directed toward face 11 where it strikes a reflective surface 26of prismatic groove 14 at point P₁₀₂. The corresponding segment of rayR₁₁₀ propagating between points P₁₀₁ and P₁₀₂ is denoted as segment 17.

Face 26 represents the working aperture of prismatic groove 14 and isconfigured to redirect ray R₁₁₀ from its original direction ofpropagation in waveguide 4 into a different direction at which ray R₁₁₀can be extracted from waveguide 4. In order to achieve this, face 26 isinclined at a slope angle θ₃₀ with respect to face 11. Accordingly, face26 makes angle θ₁₃₅ with a surface normal direction 15 to face 11 whichis also a surface normal direction with respect to face 10 due to theparallelism of faces 10 and 11. Face 26 has a planar mirrored surfacewhich provides a low-loss specular reflection for ray R₁₁₀. However, itshould be understood that this invention is not limited to the planarconfiguration of reflective face 26. It will be appreciated that face 26can be configured with any desired shape without departing from theteachings of the present invention, for example it may comprise anysegmented or curved surface.

Ray R₁₁₀ bounces from face 10 by means of TIR, at which the angle ofreflection is equal to the angle of incidence, and continues propagatingin waveguide 4 at angle θ₁₀₁ with respect to the surface normaldirection of faces 10 and 11 until it strikes face 26 at point P₁₀₂. Aray segment 18 represents a continuation of ray R₁₁₀ when it isinternally redirected/deflected by prismatic groove 14 back intowaveguide 4 so that segment 18 forms a different angle θ₁₀₂ with respectto surface normal direction 15 of face 10. The slope of face 26 isselected so as to result in angle θ₁₀₂ being smaller than angle θ₁₀₁ andalso smaller than TIR angle θ_(C). The TIR angle θ_(C) can be definedfrom the following expression.

θ_(C)=arcsin(n ₂ /n ₁)

When ray R₁₁₀ is reflected by face 26 and further strikes face 10 fromthe inside of waveguide 4 at point P₁₀₃ it maintains the same angle θ₁₀₂with respect to a surface normal direction of face 10. Since angle θ₁₀₂is smaller than TIR angle θ_(C), ray R₁₁₀ passes through face 10 withsome refraction and with relatively small Fresnel losses defined by thedifference in refractive indexes n₁ and n₂. Ray R₁₁₀ therefore becomesdecoupled from waveguide 4 and can be further collected and collimatedby the associated lens array.

Referring again to FIG. 28, since surface normal direction 15 makes anangle of 90° with face 26, θ₁₃₅=90°−θ₃₀. Accordingly, considering thatface 26 makes an angle θ₁₃₉ with respect to segment 18 of ray R₁₁₀, thefollowing expression can be derived as a matter of optics and geometry:θ₁₀₂=θ₁₀₁−2θ₃₀. Subsequently, θ₁₀₂=θ₁₀₁−2(90°−θ₁₃₅). Thus, for example,if ray R₁₁₀ propagates in waveguide 4 so that it makes an angle of 65°with respect to surface normal 15, that is θ₁₁₀=60°, and the slope offace 26 with respect to face 11 is 27 degrees, that is θ₃₀=27° andθ₁₃₅=63°, a value of θ₁₀₂=6° is obtained. Accordingly, segment 18 willstrike face 10 at the angle of 4° with respect to a normal to face 10.If waveguide 4 is made from PMMA with the reflective index n₁ of about1.49 and the ambient medium is air with refractive index n₂ of about 1,TIR angle θ_(C) will be equal to arcsin(1/1.49) which is approximately42.155°, that is greater than angle θ₁₀₂. It follows that, in the aboveexample, θ₁₀₂<θ_(C) and therefore the condition of TIR is not met atpoint P₁₀₃ resulting in ray R₁₁₀ exiting from waveguide 4 through itsface 10.

It will be appreciated that when face 26 has a mirrored surface, byselecting a suitable slope angle θ₃₀ of reflective face 26, ray R₁₁₀ canbe directed at any desired angle with respect to surface normal 15 orfaces 10 and 11.

FIG. 29 illustrates a range of incident and reflected rays for aprismatic groove within waveguide 4. The light incident upon face 26 ata particular point of an individual prismatic groove 14 can becharacterized by a fan of incident rays having a first angular apertureA₁₁ and the redirected (e.g., reflected) light can be characterized by afan of outgoing rays having a second angular aperture A₁₂. As discussedabove, prismatic grooves 14 can be configured to receive light raysincident into its working surface at various angles and redirect therays at angles lesser than the TIR angle in relation with faces 10 and11. Thus, prismatic grooves 14 can be configured to receive light from afirst angular aperture A₁₁ and redirect that light into a second angularaperture A₁₂ so that apertures A₁₁ and A₁₂ do not intersect and each rayin the second angular aperture A₁₂ propagates at an angle lesser thanangle θ_(C) with respect to surface normal direction 15 providing forthe maximum decoupling efficiency. When deflecting means employ a planarreflective face 26, the angular value of second angular aperture A₁₂will generally be the same as angular value of first angular apertureA₁₁. However, face 26 can also be made concave or convex resulting inthe second angular aperture A₁₂ being greater or smaller than the firstangular aperture A₁₁.

Toward maximizing the efficiency of light decoupling from waveguide 4and considering a planar configuration of face 26, an optimum range ofacceptable values for slope angle θ₃₀ can be selected in response to thefollowing reasoning. Since light rays are randomly distributed inwaveguide 4, ray R₁₁₀, when striking face 26, can make angles +θ_(r) inresponse to an approach to prismatic groove 14 from face 10, or of−θ_(r) in response to an approach to prismatic groove 14 from face 11,with respect to prevailing plane of the material. Therefore, face 26should be positioned to decouple ray R₁₁₀ incident into it at eitherθ_(r) or −θ_(r) with respect to the material plane. As a matter ofoptics, this condition can be written in the form of the followingexpression.

(θ_(r)+θ_(C))/2≤θ₃₀≤90°−(θ_(r)+θ_(C))/2

Referring now to both FIG. 28 and FIG. 29, in order to decouple theentire fan of rays confined within angular aperture A₁₁, slope angle θ₃₀should be within the following range:A₁₁/4+θ_(C)/2≤θ₃₀≤90°−A₁₁/4−θ_(C)/2. If slope angle θ₃₀ is outside ofthis range, a portion of the light beam redirected by the respectiveprismatic groove 14 will undergo TIR at face 10 and will thereforeremain in waveguide 4 until it can be extracted by other prismaticgrooves 14. However in the case of slope angle θ₃₀ being outside of thisrange, a longer optical path, and thus a longer waveguide 4, may berequired for decoupling all the light.

By taking the above exemplary case with waveguide 4 comprising PMMAmaterial (n₁≈1.49) with air cladding (n₁≈1) and assuming angularaperture A₁₁ of the fan of rays incident into prismatic groove 14 being60° (±30° from the plane of the material), a desired range for slopeangle θ₃₀ can be obtained as: 36.08°≤θ₃₀≤53.92° which provides over 22°wide useful span of slope angles for obtaining the maximum lightdecoupling efficiency with a minimum number of prismatic grooves 14.

Obviously, the greater aperture A₁₁ the narrower the optimum range ofangles θ₃₀ is. In an extreme case when A₁₁=2 θ_(r max), for instancewhen the light beam injected into waveguide 4 can comprise rays makingangles of up to 90°−θ_(C) with respect to the prevailing material plane,or down to θ_(C) with respect to a surface normal direction in relationto the material plane and faces 10 and 11, by making the respectivesubstitutions to obtain the following:

(2(90°−θ_(C)))/4+θ_(C)/2≤θ₃₀≤90°−(2(90°−θ_(C)))/4−θ_(C)/2,

which translates into: 45°≤θ₃₀≤45° or simply θ₃₀=45°.

In other words, face 26 should be inclined at an angle of 45° withrespect to faces 10 and 11 to decouple the maximum number of rays whenaperture A₁₁=2 θ_(rmax).

It will be appreciated by those skilled in the art that reflective facescan reflect at least a portion of the incident light by means of TIR andin which case no mirror coating may be required for face 26. Referringto FIG. 28, when face 26 makes a sufficiently acute angle with respectto segment 17, angle θ₁₂₉ can exceed a TIR angle for the opticalinterface formed by face 26 and the outside media. Thus, ray R₁₁₀ willundergo TIR at face 26 even if face 26 is optically transparent and notspecularly reflective.

Although FIG. 26 through FIG. 29 illustrated illuminator embodimentsemploying prismatic grooves with a sloped reflective face, the inventionis not limited to this configuration. The following describes a fewvariations which can be considered separately or in combination with oneanother and the other embodiments described herein.

FIG. 30A illustrates an individual v-shaped prismatic groove 14 which isconfigured to redirect and decouple the light from waveguide 4 as abifacial prismatic groove 14. Furthermore, prismatic groove 14 can haveany other geometry and any desired number of faces that can reflect,refract, scatter or otherwise redirect light propagating withinwaveguide 4 so that the redirected light can be extracted from thewaveguide.

FIG. 30B illustrates an example embodiment in which several smallerv-shaped prismatic grooves are disposed within the waveguide instead ofa single prismatic groove 14. Faces 26 of the grooves are inclined inaccordance with the above principles to allow for efficient lightextraction from waveguide 4 with the subsequent collimation by arespective lenslet 6.

FIG. 30C illustrates an example of a deflection structure 14 opticallycoupled to surface 11. The deflection structure 14 comprises a groovewith face 26. As with the foregoing embodiments, reflective face 26 isinclined at a suitable angle to decouple the light propagating inwaveguide 4. The material in which prismatic groove 14 is formed can beselected to approximately match that of waveguide 4 in which case theparasitic reflections at the interface between prismatic groove 14 andwaveguide 4 can be minimized thus minimizing the light propagationlosses.

FIG. 30D illustrates an example embodiment of a prismatic featureprotruding from face 11 which provides the same basic operation asdescribed above.

FIG. 30E illustrates an example embodiment in which the prismatic groove14 is replaced with one or more diffraction gratings (e.g., which may beproduced in the form of a hologram) and which is configured fordeflecting the incident light at a suitable angle with respect to faces10 and 11 so that the light can be effectively decoupled from waveguide4. The hologram can be produced in the form of a glass plate or highlytransparent plastic film and can be made angularly and/or spectrallymultiplexed.

The foregoing embodiments of the present invention are described uponthe case where prismatic grooves 14 are formed in or associated withface 11. However, this invention is not limited to this and can beapplied to the case when prismatic grooves 14 can positioned anywhere ator between faces 10 and 11, or they can be made embedded or integral towaveguide 4 or attached externally to either face 10 or 11, providedthat prismatic grooves 14 are optically coupled to waveguide 4 and canintercept a portion of the light propagating in waveguide 4 and extractthe light from the waveguide to allow for the subsequent collimationwith lenses 6.

FIG. 31 illustrates an example embodiment in which the prismatic grooves14 are formed in face 10, which is the opposite planar face as thatdescribed in the embodiments described above. Referring to the ray R₁₁₀propagating in waveguide 4 strikes prismatic groove 14 at angle θ₁₀₁with respect to a surface normal direction 15 of face 10. Prismaticgroove 14 deflects segment 117 of ray R₁₁₀ into segment 118 which formsangle θ₁₀₂ with respect to surface normal direction 15. Light prismaticgroove 14 is configured to have both a reflective face 26 and atransparent face 55. Ray R₁₁₀ passes through face 55 and is reflected byface 26 toward a corresponding lens 6. Face 26 is inclined with respectto face 10 so as to provide a suitable angle θ₁₀₂ for segment 118.Similarly to the embodiments illustrated above, ray R₁₁₀ exits waveguide4 and is collected and collimated by lens array 5. Face 55 can be madeapproximately perpendicular to face 10 or it can be inclined at anysuitable angle with respect to face 10 or surface normal direction 15,toward providing a more efficient light deflection or extraction fromwaveguide 4.

FIG. 32 illustrates an example embodiment in which the extraction of theray is facilitated without the need of a reflective deflection. In thepreceding embodiments of the present invention a prismatic groove 14 wasconfigured with a reflective face 26. However, the present invention isnot limited to this configuration. The figure depicts an example inwhich a prismatic groove 14 (or ridge) of a refractive type is utilizedin which light passes through face 26 (with deflection) rather thanbeing reflected from it. In FIG. 32 a prismatic feature protrudes fromsurface 11 with prismatic face 26 that is inclined with respect tosurface 10 at a suitable angle so that the condition of TIR is not metfor ray R₁₁₀ when it strikes face 26 and, therefore, ray R₁₁₀ isextracted from waveguide 4 for subsequent collimation.

It should be appreciated that the illumination device can be configuredto collect light rays in a preselected spectral domain and/or only thoserays propagating in waveguide 4 in a predetermined range of acceptanceangles. For example, prismatic grooves 14 can be replaced by areflection or transmission hologram designed to deflect and decoupleonly a specific wavelength or a relatively narrow range of wavelengthsfrom waveguide 4 while allowing the other wavelengths to furtherpropagate through waveguide 4 by means of TIR. Alternatively, one ormore layers of a dichroic material can be deposited on face 26 ofprismatic groove 14 which will cause the incident light to be split upinto distinct beams of different wavelengths and allow only selectedbeam(s) to be extracted from waveguide 4. In a further example,prismatic grooves 14 can be designed so that any rays impinging onto itsactive aperture within an acceptance angle of up to a pre-determinedvalue (e.g., up to 30 degrees) will be extracted from waveguide 4. Theremainder of the light rays are allowed to propagate further inwaveguide 4 at angles greater than TIR angle θ_(C) with respect tonormal 15 and these latter rays can therefore be allowed to remain inwaveguide 4.

FIG. 33 illustrates an example embodiment in which the waveguide andcollimator are not separated by air. It should be appreciated that thepresent invention is not limited to configurations in which thewaveguide is separated from the lens array (collimator) by a medium ofair. The figure depicts a practical embodiment of the present inventionwhich incorporates a buffer layer 19 of optically transmissive materialhaving a refractive index lower than that of waveguide 4. Layer 19 isseparating waveguide 4 from lens array 5 providing for a stepped drop inrefractive index outwardly from waveguide 4 so that light can be trappedin the waveguide by TIR and that the illuminator device 2 has the samebasic operation as discussed above. Layer 19 can be positioned betweenlens array 5 and waveguide 4 so that system 2 forms a monolithicsandwiched structure. Suitable materials for layer 19 can be selectedfrom the group of low refractive index materials consisting essentiallyof, but not limited to: monomers, polymers, fluoropolymers, low-noptical adhesives, thin films, materials commonly used for cladding inoptical waveguides or any other optically clear material provided thatits refractive index is lower than the refractive index of the materialselected for waveguide 4. Additionally, amorphous fluoropolymers whichare conventionally used for cladding optical waveguides such as PFTE AF1600 and PFTE AF 2400 are particularly well suited for use.

Additionally, face 11 of waveguide can be provided with a backsheet orcladding layer 20 which also has a low refractive index so thatwaveguide 4 is encapsulated and protected from the outside media by alow-n material similar to conventional light guides. This can help avoidlight spillage from waveguide 4 and improve the efficiency of system 2.Cladding materials suitable for layer 20 can include any of the low-nmaterials mentioned above for layer 19. Alternatively, layer 20 can beformed by a plastic reflective film or by metallization of face 11 toimprove reflectivity or reduce light spillage through face 11. Anotherexample of a suitable protective backsheet material for layer 20 can bePolyvinyl fluoride (PVF), a fluoropolymer which is commerciallyavailable as a film from DuPont and is sold under the Tedlar® brand.

Similarly, any or all side faces (side walls) or terminal faces (endwalls, terminal walls) of waveguide 4 can be encapsulated or otherwisecovered by a protective or reflective layer and allowed to reflect lightpropagating in waveguide 4 back into the waveguide by means of TIR orspecular reflection. It will be appreciated that layer 20 orencapsulation layers of the edges of waveguide 4 do not have to beoptically transparent and can include opaque, light scattering orreflective materials. Yet further, optical illumination device 2 canincorporate any other suitable layers such as reflective oranti-reflective coatings, diffusers, radiation protective coatings orfilms, scratch and stain resistant coatings, light filtering films andthe like. By way of example, waveguide 4, lens array 5 or any of theirportions can be coated by dip coating, spin coating, vacuummetallization, applying a thin film using low-n adhesives, etc.

In accordance with an embodiment of the present invention, opticalillumination device 2 discussed above can comprise an elongated lightsource extending along terminal face 35 for inputting light intowaveguide 4. Alternatively, a plurality of miniature light sources canbe arranged along face 35 for this purpose.

The foregoing embodiments are described upon the case when prismaticgrooves 14 are aligned pair wise with the respective lenses 6 which canbe preferred for collimating the light decoupled from waveguide 4 into ahighly collimated, particularly parallel, beam. However, this inventionis not limited to this configuration and can also be implemented so thatthe optical axis of each individual prismatic groove 14 is slightlyoffset with respect to an optical axis of the matching lens 6.Furthermore, the amount of the offset can be varied for differentprism-lens pairs over the length of waveguide 4. Particularly, prismaticgrooves 14 and lenslets 6 can be positioned and aligned in accordance toa pre-selected ordered or randomized pattern. This can be useful, forexample to create a non-parallel, yet collimated beam with a desiredangular spread and or a particular intensity distribution. By way ofexample, the plurality of lenses 6 can be designed to direct therespective beams into converging directions or focus. Alternatively,these directions can be made diverging to distribute the illuminationpattern within a pre-determined angle (a diverging conical lightpattern). The respective beams of light can be spaced apart, overlapped,or mixed in any suitable manner so as to provide the desired operationor light distribution in space or on a target.

FIG. 34 illustrates an example embodiment in which light is deflectedfor exiting the waveguide and being collimated on both sides of thewaveguide. Although, the foregoing embodiments described the use ofprismatic grooves disposed on a single side of the waveguide, it shouldbe appreciated that the present invention is not limited to thatconfiguration. The figure depicts grooves 14 formed in face 10 and face11 with a respective lens array 5 on either side of waveguide 4 in abifacial configuration of optical device 2.

FIG. 35 illustrates an embodiment of a space efficient optical device 2in which matching pairs of prismatic grooves 14 and lenses 6 aredisposed in a two-leg symmetric configuration along planar waveguide 4.There is a central opening in waveguide 4 in which light source 145 isinserted so that the latter can illuminate the waveguide as illustratedin the figure. In the illustrated case, source 145 may comprise aside-emitting LED for maximizing the efficiency of injecting the lightinto waveguide 4. A suitable finned or finless heat sink can be furtherattached to source 145 for improved heat removal. In FIG. 35 a finnedheat sink 54 is shown conforming to the planar geometry of waveguide 4.Common materials for heat sink 54 may comprise, for instance, aluminum,copper, and any of their alloys or similar materials. A layer of opticaladhesive or encapsulant such as silicone, EVA resin or the like can beprovided between light source 145 and waveguide 4 to promote optical andphysical contact. Toward efficient light injection, the refractive indexof the adhesive or encapsulant should preferably be close to, or greaterthan, the refractive index of the material of waveguide 4. Waveguide 4distributes the injected light along its working aperture where thelight is decoupled, one portion at a time, by prismatic grooves 14 andcollimated into a quasi-parallel beam by respective lenses 6 similarlyto the process described above.

Referring again to FIG. 35, system 2 can be arranged to have either alinear configuration with a plane of symmetry perpendicular to thedrawing plane, similarly to the embodiments described above, or to havean annular configuration. In an annular configuration, optical device 2can have an axial symmetry in which case the shapes of lens array 5 andwaveguide 4 can be formed by a revolution of the cross sectional designshown in FIG. 35 around an axis of symmetry by a full or partial angularturn.

FIG. 36A through FIG. 36D illustrate exemplary configurations of theilluminator, such as linear and various circular, and partial patterns.In each case light rays are shown entering waveguide 4 in the areaindicated as a light input area 147. It should also be understood thatoptical device 2 can be configured to have multiple light input areas147 with multiple light sources 145. In addition, either one or bothwaveguide 4 and lens array 5 may be tapered and or provided with anyother desired shape.

FIG. 37A through 37B illustrate an example embodiment of a roundaxisymmetrical configuration. While a partial-circle configuration ofoptical device 2 is shown in the figures for the sake of clarity ofexplanation, it should be understood that lens array 5 and waveguide 4,along with respective lenses 6 and prismatic grooves 14, more preferablyspan a full-circle annular configuration. Alternatively, the device canbe configured into any desired symmetric or asymmetric shape, or partialshape, such as cutting from an annular configuration, such as forexample, a rectangular shape (see, e.g., FIG. 36C and FIG. 36D), orvarious decorative shapes.

Although the foregoing embodiments of the illuminator are discussing aplanar configuration, the invention is not limited to planar lightcollection devices. It can also be applied to a case when collectorarray 5 and waveguide 4 are made of a flexible material such thatoptical device 2 is able to bend and can be shaped, for example, in acylindrical configuration.

It should also be understood that this invention is not limited toemploying lenses 6 of an imaging type and can be applied to the casewhen lenses 6 can have any other suitable shape, so that an individuallens 6 can produce a convergent or divergent beam or any other lightpattern. Furthermore, this invention is not limited to the use of lensarray 5 of a refractive type and can also be applied to the case whenlens array 5 can be replaced by a reflective mirror array. By way ofexample, collector array 5 can be formed by a dense planar array ofmicro-mirrors in which case each mirror element 6 can be represented bya concave reflector which has a mirrored surface and is configured tofocus an incident beam of light onto a respective prismatic grooves 14.Each mirror can have a spherical shape, parabolic shape or any othershape resulting in collection of the incident light to a substantiallysmaller area than the aperture area of the mirror. In another example,each mirror in collector array 5 can, in turn, be formed by amicro-array of planar reflectors inclined at suitable angles, such as aFresnel mirror, so as to result in efficient focusing the incidentradiation.

FIG. 38 illustrates an example embodiment of optical illuminator device2 in which collector array 5 comprises a planar transparent body havinga surface texture in the form of a densely packed array of micro-mirrors6. Thus, each micro-mirror 6 is integral to the planar transparent body.Each micro-mirror 6 has a curved mirrored surface that allows it toefficiently collect incident light and focus the light onto acorresponding prismatic groove 14 having a substantially smalleraperture. In a similar manner as lenses in lens array 5, micro-mirrorscan be designed in linear or point focus configurations. Waveguide 4 isconfigured in the form of a planar transparent plate having a refractiveindex greater than that of the outside media and optically coupled toeach of the plurality of prismatic grooves 14 associated with face 11.Both parallel faces 10 and 11 of waveguide 4 are also preferablytransparent to incident light. Similarly to the examples discussedabove, each prismatic groove 14 comprises reflective face 26.

In operation, incident ray R₁₀₁ enters waveguide 4, propagates inwaveguide 4 by means of TIR and enters prismatic groove 14. Face 26 isinclined with respect to a normal to walls 10 and 11 and it redirectsray R₁₀₁ back into waveguide 4 at an angle with respect to a normal towalls 10 and 11 which is less than critical angle θ_(C) so that ray R₁₀₁is decoupled by prismatic groove 14 and directed to a respectivemicro-mirror 6. In turn, micro-mirror 6 directs ray R₁₀₁ to a directionperpendicular to wall 11. Accordingly, rays R₁₀₂, R₁₀₁ and R₁₀₂propagating in waveguide 4 are also decoupled from waveguide 4 anddirected generally toward the same direction. In similar manner to thesystem of FIG. 33, transparent cladding or buffer layer 19 can beconfigured with low-n material can be laid between the collector array 5and waveguide 4. Further, a cladding and/or protective layer or layerscan be added to either or all of the walls or faces of waveguide 4 toprotect it from the environment. Further details of operation of device2 shown in FIG. 38 as well as its possible variations configurationswill be apparent from the foregoing description of preferred and otherembodiments.

It should be noted that any other conventional device used to collect orcollimate light can be used in place of lenses 6. Any known opticalsystem or collector of radiant energy or light which collects the energyfrom it entrance aperture and directs it further with improvedcollimation can be used for the purpose of this invention. Illustrativeof useful devices that can be used in place of lenses 6 are spherical oraspherical refractive lenses, parabolic or spherical mirrors, Fresnellenses, Total Internal Reflection (TIR) lenses, gradient index lenses,diffraction lenses, lens arrays, mirrors, Fresnel mirrors, mirror arraysand the like.

The foregoing embodiments have been described upon the case whenv-shaped prismatic grooves 14 are used for decoupling the light fromwaveguide 4. However, this invention is not limited to this and can beapplied to the case when any suitable optical device used to receive thelight beam in a pre-determined acceptance angle from one direction anddeflect at least a substantial portion of the incident beam from itsoriginal direction to a different direction can be utilized in place ofprismatic grooves 14. Each such optical element should be configured tointercept a portion of the light propagating within waveguide 4 andredirect it at a different propagation angle with respect to faces 10and/or 11 at which the condition of TIR is not met and the light canexit waveguide 4 and can further be collected and collimated byrespective lens 6. By means of example, an alternative to prismaticgrooves 14 can include a reflective surface or a refractive elementdisposed at an angle to the incident light beam and optically coupled towaveguide 4. Similarly, an alternative can include planar or curvedmirrors, prisms, prism arrays, diffraction gratings, holograms, andsimilar optical elements. Additionally, various light scattering orlight diffusing elements, such as small areas of waveguide 4 paintedwith a white paint or provided with matte-finish, can be used in placeof prismatic grooves 14 which will redirect at least a portion of lightout of waveguide 4 through at least one of its faces 10 or 11 so thatoptical device 2 will have the same basic structure and operation.

The present invention is not limited to the case when waveguide 4 andlens array 5 are disposed in a stationary position with respect to eachother and can also be applied to the case when lens array 5 andwaveguide 4 can be disposed in any one of a translated, a reversedand/or a rotated orientation relative to each other in order, forexample, to achieve different collimation angles or desired visualeffects for the collimated light. Furthermore, lens array 5 andwaveguide 4 can be made movable with respect to each other to providefor fine tuning or “focusing” the collimated beam.

Accordingly, it will be appreciated that the system of the presentinvention can be used for collecting and concentrating otherwisedistributed light in a very space-efficient manner by using a thinplanar geometry of the light collecting optics. Furthermore, the systemallows for homogenizing the collected light by means of multiplelossless total internal reflections and delivering the light to an edgeof a waveguide with a substantial concentration and low loss.

Additionally, the device of this invention can be used for collimatingotherwise divergent light in a very space-efficient manner by using athin planar geometry of the collimating optics. Furthermore, the deviceallows distributing light emitted by a highly localized light sourceacross a much larger area and creating a broad yet highly collimatedlight beam without the glare typically associated with bright pointsources such as high-power LEDs, incandesced lamps and the like.

As can be seen, therefore, the present invention can be implemented invarious ways, which can include, but which are not limited to, one ormore of the following embodiments, modes and features described herein:

1. An apparatus for light collimation and distribution, comprising: aplanar waveguide having an optically transparent planar material havingedges disposed between a first planar surface and a second planarsurface; in which said planar waveguide is configured to receive lighton one edge of said planar material, and to propagate the received lightthrough said planar waveguide in response to optical transmission andtotal internal reflection; a plurality of light collimating elementswithin a collimating array which is disposed in an optical receivingrelationship with a planar surface of said planar waveguide; and aplurality of light deflecting elements optically coupled to saidwaveguide and configured for deflecting light propagating through saidplanar waveguide at a sufficiently low angle, below the predeterminedcritical angle for total internal reflection (TIR), with respect to asurface normal direction of an exterior surface of said planar waveguideto exit said planar waveguide and enter said collimating array; whereineach of said plurality of light deflecting elements is in apredetermined alignment with each of said plurality of light collimatingelements; wherein light received on the edge of said planar waveguide isangularly redirected, collimated, and distributed from the surface ofsaid collimating array which is optically coupled to said planarwaveguide.

2. The apparatus of embodiment 1, wherein said plurality of lightcollimating elements comprises a parallel array of elongated lenticularlenses.

3. The apparatus of embodiment 1, wherein said plurality of lightcollimating elements comprises a parallel array of elongated focusmirrors.

4. The apparatus of embodiment 1, wherein said plurality of lightdeflecting elements comprises a parallel array of elongated grooves.

5. The apparatus of embodiment 1, wherein said plurality of lightdeflecting elements comprises a parallel array of elongated grooves;wherein said grooves are configured at a slope angle which is bounded bythe relation in which is the refractive index of the planar waveguideand is the refractive index of the collimator array.

6. The apparatus of embodiment 1, wherein said plurality of lightdeflecting elements comprises grooves within said planar waveguideconfigured for redirecting the received light in response to reflectionfrom at least one surface of said groove toward said collimating array.

7. The apparatus of embodiment 1: wherein said light deflecting elementscomprise grooves; and wherein said grooves are formed within each of aplurality of blocks that are attached and in optical communication withsaid planar waveguide, and said grooves are configured for redirectingthe received light in response to reflection from at least one surfaceof said groove toward said collimating array.

8. The apparatus of embodiment 1: wherein said light deflecting elementscomprise grooves; and wherein each of said grooves has a transparentsurface and a reflective surface, and light received from the planarwaveguide passes through the transparent surface of each of said groovesto be reflected from the reflective surface of each of said groovestoward said collimating array.

9. The apparatus of embodiment 1: wherein said light deflecting elementscomprise grooves; and wherein each of said grooves comprise a prismaticgroove or ridge formed in a surface of said planar waveguide disposedtoward said collimating array for refractively deflecting the receivedlight impinging on said prismatic groove to pass through said prismaticgroove or ridge to exit the planar waveguide.

10. The apparatus of embodiment 1, wherein said plurality of lightcollimating elements is selected from the group of optical elementsconsisting of imaging lenses, non-imaging lenses, spherical lenses,aspherical lenses, lens arrays, Fresnel lenses, TIR lenses, gradientindex lenses, diffraction lenses, mirrors, Fresnel mirrors, sphericalmirrors, parabolic mirrors, mirror arrays, and trough mirrors.

11. The apparatus of embodiment 1, wherein said plurality of lightdeflecting elements is selected from the group of optical elementsconsisting of planar mirrors, curved mirrors, prisms, prism arrays,prismatic grooves, surface relief features, reflective surfaces,refractive surfaces, diffraction gratings, holograms, and lightscattering elements.

12. The apparatus of embodiment 1, further comprising an opticalinterface disposed between said planar waveguide and said collimatingarray; wherein said optical interface is characterized by a drop inrefractive index in the direction of light propagation from said planarwaveguide toward said collimating array.

13. The apparatus of embodiment 1, further comprising: an opticalinterface layer disposed between said planar waveguide and saidcollimating array; wherein said optical interface layer is selected fromthe group of optical materials consisting of low refractive indexmonomers, polymers, fluoropolymers, low-n optical adhesives, thin films,and optical waveguide cladding materials.

14. The apparatus of embodiment 1, further comprising: an opticalinterface layer disposed between said planar waveguide and saidcollimating array; wherein said optical interface layer has a lowerrefractive index than said planar waveguide.

15. The apparatus of embodiment 1, further comprising: an opticalinterface layer disposed between said planar waveguide and saidcollimating array; wherein said optical interface layer comprises air.

16. The apparatus of embodiment 1, further comprising at least oneillumination source coupled to at least one edge of said planarwaveguide.

17. The apparatus of embodiment 1, further comprising at least oneillumination source optically coupled to edges of a cutout within saidplanar waveguide.

18. The apparatus of embodiment 1, wherein both said collimating arrayand said planar waveguide have a round or sectorial shape obtainable bya revolution of a cross section of said collimating array and saidplanar waveguide around an axis.

19. The apparatus of embodiment 1, wherein said collimator arraycomprises point focus lenses.

20. The apparatus of embodiment 1: wherein said collimator arraycomprises point focus lenses; and wherein said point focus lenses have ashape selected from the group consisting of round, rectangular, square,and hexagonal.

21. The apparatus of embodiment 1, wherein said collimator arraycomprises point focus mirrors.

22. The apparatus of embodiment 1: wherein said collimator arraycomprises point focus mirrors; and wherein said point focus mirrors havea shape selected from the group of shapes consisting of round,rectangular, square, and hexagonal.

23. The apparatus of embodiment 1, wherein said planar waveguidecomprises a rectangular plate having a first terminal edge, a secondterminal edge, a first side wall, a second side wall, said first planarsurface and said second planar surface.

24. The apparatus of embodiment 1, further comprising: a mirroredsurface; wherein said planar waveguide comprises a rectangular platehaving a first terminal edge, a second terminal edge, a first side wall,a second side wall, said first planar surface and said second planarsurface; and wherein said mirrored surface is on one or more of saidfirst terminal edge, said second terminal edge, said first side wall andsaid second side wall.

25. The apparatus of embodiment 1, further comprising: a cladding layer;wherein said planar waveguide comprises a rectangular plate having afirst terminal edge, a second terminal edge, a first side wall, a secondside wall, said first planar surface and said second planar surface; andwherein said a cladding layer is disposed upon one or more of said firstterminal edge, said second terminal edge, said first side wall and saidsecond side wall.

26. The apparatus of embodiment 1, wherein said planar waveguide andsaid collimator array are adapted for being retained in either a planarconfiguration or in bent and/or rolled configurations.

27. The apparatus of embodiment 1, wherein said planar waveguide andsaid collimator array are adapted for being retained in a translated, areversed and/or a rotated orientation relative to each other towardachieving a adjusting the light distribution or collimation pattern.

28. The apparatus of embodiment 1, wherein said planar waveguide andsaid collimator array are adapted for being retained in a movablerelationship with one another toward adjusting the light distribution orcollimation pattern.

29. The apparatus of embodiment 1, further comprising: a coating on theexterior of said planar waveguide and/or said collimator array; whereinsaid coating is selected from the group of coatings consisting ofanti-reflective, protective, encapsulates, reflective, diffusive,radiation protective, scratch and stain resistant, and light filtering.

30. An apparatus for light collimation and distribution, comprising: aplanar waveguide having an optically transparent planar materialconfigured to receive light on one edge of said planar material, and topropagate the received light through said planar waveguide in responseto optical transmission and total internal reflection; a parallelcollimating array having a plurality of elongated light collimatinglenses disposed in an optical receiving relationship with a planarsurface of said planar waveguide; and a parallel deflecting array havinga plurality of elongated light deflecting grooves within said planarwaveguide which are configured for deflecting light propagating throughsaid waveguide at a sufficiently low angle, below the predeterminedcritical angle for total internal reflection (TIR), with respect to asurface normal direction of an exterior surface of said planar waveguideto exit said planar waveguide and enter said parallel collimating array;wherein each of said plurality of elongated light deflecting grooves isin a predetermined alignment with each of said plurality of elongatedlight collimating lenses; wherein light received on the edge of saidplanar waveguide is angularly redirected, collimated, and distributedfrom the surface of said parallel collimating array which is opticallycoupled to said planar waveguide.

31. A method for distributing radiant energy comprising: receivingradiant energy into an edge of an optical waveguide having edgesdisposed between a first planar surface and a second planar surface;propagating the radiant energy by optical transmission and totalinternal reflection in an optical material disposed between the firstplanar surface and the second planar surface along the length of theoptical waveguide; deflecting the radiant energy at a plurality ofdeflecting elements distributed along the first planar surface and/orsecond planar surface of the optical waveguide to a sufficiently lowangle, below the predetermined critical angle for total internalreflection (TIR) which is with respect to a surface normal direction ofthe first planar surface or second planar surface of the opticalwaveguide, causing the radiant energy to exit the surface of the opticalwaveguide through the first planar surface and/or the second planarsurface; and collimating the radiant energy exiting the opticalwaveguide at a plurality of focal zones in response to the radiantenergy passing through a plurality of radiation collimating elements.

32. An apparatus for collecting light, comprising: a plurality of lightcollecting elements within a collector array configured for collectingreceived light; a planar waveguide having edges disposed between a firstplanar surface and a second planar surface; said planar waveguide isdisposed in an optical receiving relationship with said collector arrayand configured to propagate the received light by optical transmissionand total internal reflection; and a plurality of light deflectingelements optically coupled to said planar waveguide with each of saidplurality of light deflecting elements disposed in energy receivingrelationship within said planar waveguide to at least one of saidplurality of light collecting elements; wherein each of said pluralityof light deflecting elements is configured to redirect incident light ata sufficiently high angle, above the predetermined critical angle fortotal internal reflection (TIR) with respect to a surface normaldirection with respect to the first planar surface or the second planarsurface of said planar waveguide, to redirect and propagate the receivedlight within said planar waveguide by optical transmission and TIR.

33. The apparatus of embodiment 32, wherein said plurality of lightcollecting elements comprises a parallel array of elongated focusmirrors.

34. The apparatus of embodiment 32, wherein said plurality of lightcollecting elements comprises a parallel array of elongated lenticularlenses.

35. The apparatus of embodiment 32: wherein said plurality of lightdeflecting elements comprises a parallel array of elongated grooves.

36. The apparatus of embodiment 32: wherein said plurality of lightdeflecting elements comprises a parallel array of elongated grooves;wherein said grooves are configured at a slope angle θ₃₀ which isbounded by the relation

${\arcsin \left( \frac{n_{2}}{n_{1}} \right)} \leq \theta_{30} \leq {\arccos \left( \frac{n_{2}}{n_{1}} \right)}$

in which n₁ is the refractive index of the planar waveguide and n₂ isthe refractive index of an outside medium.

37. The apparatus of embodiment 32, wherein said plurality of lightdeflecting elements comprises grooves within said planar waveguideconfigured for redirecting the received light in response to reflectionfrom at least one surface of said groove into the plane of the planarwaveguide.

38. The apparatus of embodiment 32, wherein said plurality of lightdeflecting elements comprises grooves formed within each of a pluralityof blocks that are attached and in optical communication with saidplanar waveguide, and said grooves are configured for redirecting thereceived light in response to reflection from at least one surface ofsaid groove into the plane of the planar waveguide.

39. The apparatus of embodiment 32, wherein said plurality of lightdeflecting elements is selected from the group of optical elementsconsisting of planar mirrors, curved mirrors, prisms, prism arrays,prismatic grooves, surface relief features, reflective surfaces,refractive surfaces, diffraction gratings, holograms, and lightscattering elements.

40. The apparatus of embodiment 32, wherein said plurality of lightcollecting elements is selected from the group of optical elementsconsisting of imaging lenses, non-imaging lenses, spherical lenses,aspherical lenses, lens arrays, Fresnel lenses, TIR lenses, gradientindex lenses, diffraction lenses, mirrors, Fresnel mirrors, sphericalmirrors, parabolic mirrors, mirror arrays, and trough mirrors.

41. The apparatus of embodiment 32, further comprising: an opticalinterface disposed between said planar waveguide and said collectorarray; wherein said optical interface is characterized by a drop inrefractive index in the direction of light propagation from said planarwaveguide toward said collimating array.

42. The apparatus of embodiment 32, further comprising: an opticalinterface layer disposed between said planar waveguide and saidcollector array; wherein said optical interface layer is selected fromthe group of optical materials consisting of low refractive indexmonomers, polymers, fluoropolymers, low-n optical adhesives, thin films,and optical waveguide cladding materials.

43. The apparatus of embodiment 32, further comprising: an opticalinterface layer disposed between said planar waveguide and saidcollector array; wherein said optical interface layer has a lowerrefractive index than said planar waveguide.

44. The apparatus of embodiment 32, further comprising: an opticalinterface layer disposed between said planar waveguide and saidcollector array; wherein said optical interface layer comprises air.

45. The apparatus of embodiment 32, wherein said planar waveguidecomprises a rectangular plate having a first terminal edge, a secondterminal edge, a first side wall, a second side wall, said first planarsurface and said second planar surface.

46. The apparatus of embodiment 32, further comprising: a mirroredsurface; wherein said planar waveguide comprises a rectangular platehaving a first terminal edge, a second terminal edge, a first side wall,a second side wall, said first planar surface and said second planarsurface; and wherein said mirrored surface is on one or more of saidfirst terminal edge, said second terminal edge, said first side wall andsaid second side wall.

47. The apparatus of embodiment 32, further comprising: a claddinglayer; wherein said planar waveguide comprises a rectangular platehaving a first terminal edge, a second terminal edge, a first side wall,a second side wall, said first planar surface and said second planarsurface; and wherein said cladding layer is disposed on one or more ofsaid first terminal edge, said second terminal edge, said first sidewall and said second side wall.

48. The apparatus of embodiment 32, further comprising: at least oneoptically responsive electronic device; wherein said planar waveguidecomprises a rectangular plate having a first terminal edge, a secondterminal edge, a first side wall, a second side wall, said first planarsurface and said second planar surface; and wherein said at least oneoptically responsive electronic device coupled to at least one of saidfirst terminal edge and said second terminal edge of said planarwaveguide.

49. The apparatus of embodiment 32, further comprising: at least onephotovoltaic cell; wherein said planar waveguide comprises a rectangularplate having a first terminal edge, a second terminal edge, a first sidewall, a second side wall, said first planar surface and said secondplanar surface; and wherein said at least one photovoltaic cell iscoupled to at least one of said first terminal edge and said secondterminal edge of said planar waveguide.

50. The apparatus of embodiment 32, further comprising at least oneoptically responsive electronic device coupled to edges of a cutoutwithin said planar waveguide.

51. The apparatus of embodiment 32, further comprising: at least onelight harvesting area configured for outputting collected receivedlight; wherein the area of said light harvesting area is smaller thanthe area of the collector array; wherein said planar waveguide comprisesa rectangular plate having a first terminal edge, a second terminaledge, a first side wall, a second side wall, said first planar surfaceand said second planar surface; and wherein any cladding layer orprotective layers disposed upon said light harvesting area on one ormore of said first terminal edge, said second terminal edge, said firstside wall and said second side wall, is removed for harvesting thelight.

52. The apparatus of embodiment 32, wherein both said collector arrayand said planar waveguide have a round or sectorial shape obtainable bya revolution of a cross section of said collector array and said planarwaveguide around an axis.

53. The apparatus of embodiment 32, wherein said collector arraycomprises point focus lenses.

54. The apparatus of embodiment 32: wherein said collector arraycomprises point focus lenses; and wherein said point focus lenses have ashape selected from the group consisting of round, rectangular, square,and hexagonal.

55. The apparatus of embodiment 32, wherein said collector arraycomprises point focus mirrors.

56. The apparatus of embodiment 32, wherein said planar waveguide andsaid collector array are adapted for being retained in either a planarconfiguration or in bent and/or rolled configurations.

57. The apparatus of embodiment 32, wherein said planar waveguide andsaid collector array are adapted for being retained in a translated, areversed and/or a rotated orientation relative to each other towardadjusting the acceptance angle or for tracking the source of light.

58. The apparatus of embodiment 32, wherein said planar waveguide andsaid collector array are adapted for being retained in a movablerelationship with one another toward adjusting acceptance angle or fortracking the source of light.

59. The apparatus of embodiment 32, further comprising: a coating onsaid planar waveguide and/or said collector array; wherein said coatingis selected from the group of coatings consisting of anti-reflective,protective, encapsulates, reflective, diffusive, radiation protective,scratch and stain resistant, and light filtering.

60. An apparatus for collecting light, comprising: a parallel collectingarray having a plurality of elongated light collecting structuresconfigured for collecting received light; a planar waveguide havingedges disposed between a first planar surface and a second planarsurface; said planar waveguide is disposed in an optical receivingrelationship with said collector array and configured to propagate thereceived light by elements of optical transmission and total internalreflection; and a parallel deflecting array having a plurality of lightdeflecting groove structures optically coupled to said planar waveguidewith each of said plurality of light deflecting groove structuresdisposed in light receiving relationship within said planar waveguide toat least one of said light collecting structures; wherein each of saidplurality of light deflecting groove structures is configured toredirect incident light at a sufficiently high angle, above thepredetermined critical angle for total internal reflection (TIR) withrespect to a surface normal direction of an exterior surface of saidplanar waveguide, to redirect and propagate the received light withinsaid planar waveguide by optical transmission and TIR.

61. A method for collecting radiant energy comprising: concentrating aradiant energy received upon a plurality of focal zones in response to aplurality of radiation concentrator elements; directing the radiantenergy from said plurality of focal zones through a first planar surfaceinto an optical waveguide having edges disposed between a first planarsurface and a second planar surface; deflecting the radiant energy at aplurality of deflecting elements positioned to received the radiantenergy from the focal zones, and to deflect the radiant energy into theplanar waveguide at angles exceeding the critical angle of totalinternal reflection in said waveguide, which is with respect to asurface normal direction of the first planar surface or second planarsurface of the optical waveguide; and propagating said radiant energythrough said optical waveguide by optical transmission and totalinternal reflection.

Although the description above contains many details, these should notbe construed as limiting the scope of the invention but as merelyproviding illustrations of some of the presently preferred embodimentsof this invention. Therefore, it will be appreciated that the scope ofthe present invention fully encompasses other embodiments which maybecome obvious to those skilled in the art, and that the scope of thepresent invention is accordingly to be limited by nothing other than theappended claims, in which reference to an element in the singular is notintended to mean “one and only one” unless explicitly so stated, butrather “one or more.” All structural, chemical, and functionalequivalents to the elements of the above-described preferred embodimentthat are known to those of ordinary skill in the art are expresslyincorporated herein by reference and are intended to be encompassed bythe present claims. Moreover, it is not necessary for a device or methodto address each and every problem sought to be solved by the presentinvention, for it to be encompassed by the present claims. Furthermore,no element, component, or method step in the present disclosure isintended to be dedicated to the public regardless of whether theelement, component, or method step is explicitly recited in the claims.No claim element herein is to be construed under the provisions of 35U.S.C. 112, sixth paragraph, unless the element is expressly recitedusing the phrase “means for.”

What is claimed is:
 1. An edge-lit waveguide illumination system,comprising: an optically transmissive plate having a flexible monolithicstructure, a front surface, an opposing back surface extending parallelto the front surface, a first edge, a second edge extending parallel tothe first edge, a third edge extending perpendicular to the first andsecond edges, and a fourth edge extending parallel to the third edge,wherein a distance between the first and second edges is at least 40times greater than a thickness of the optically transmissive plate and adistance between the third and fourth edges is at least 20 times greaterthan the thickness of the optically transmissive plate; a plurality oflight emitting diodes optically coupled to the first edge and configuredto emit a divergent light beam towards the first edge; a lenticulararray of linear cylindrical lenses formed in the front surface andextending along straight parallel lines between two opposing edges ofthe optically transmissive plate; a plurality of discrete lightextracting surface relief features formed in the back surface accordingto a two-dimensional pattern such that individual ones of the pluralityof the discrete light extracting surface relief features are separatedfrom each other and from each of the first, second, third, and fourthedges by smooth and planar portions of the back surface; a reflectivesurface approximately coextensive with the optically transmissive plateand positioned on a back side of the optically transmissive plate; and alight diffusing layer approximately coextensive with the opticallytransmissive plate, wherein the optically transmissive plate isconfigured to receive light on the first edge, guide the light receivedon the first edge towards the second edge using optical transmission andtotal internal reflection, and distribute the light received on thefirst edge from both the front and back surfaces towards divergentdirections, wherein the optically transmissive plate is furtherconfigured to receive light on the front surface and propagate the lightreceived on the front surface towards the back surface, wherein an areaoccupied by each of the linear cylindrical lenses is substantiallygreater than an area occupied by each of the plurality of the discretelight extracting surface relief features, and wherein at least one ofthe plurality of discrete light extracting surface relief features isconfigured to disrupt total internal reflection at the back surface andextract at least some light propagated in the optically transmissiveplate towards the reflective surface.
 2. An edge-lit waveguideillumination system as recited in claim 1, wherein at least some of thediscrete light extracting surface relief features have randomizedpositions within the two-dimensional pattern.
 3. An edge-lit waveguideillumination system as recited in claim 1, wherein at least some of theplurality of discrete light extracting surface relief features arearranged in parallel rows and columns within the two-dimensionalpattern.
 4. An edge-lit waveguide illumination system as recited inclaim 1, further comprising a light filtering film.
 5. An edge-litwaveguide illumination system as recited in claim 1, wherein at leastone of the plurality of discrete light extracting surface relieffeatures is configured to deflect at least some light using totalinternal reflection and direct the deflected light towards the linearcylindrical lenses at an angle of less than 42 degrees with respect to anormal to the back surface.
 6. An edge-lit waveguide illumination systemas recited in claim 1, wherein at least one of the plurality of discretelight extracting surface relief features comprises a cavity formed inthe back surface and having a curved wall, wherein the curved wall isconfigured to deflect light using both total internal reflection andrefraction.
 7. An edge-lit waveguide illumination system as recited inclaim 1, wherein at least one of the plurality of discrete lightextracting surface relief features comprises a light scattering materialand has a textured surface.
 8. An edge-lit waveguide illumination systemas recited in claim 1, wherein at least one of the plurality of discretelight extracting surface relief features comprises a light diffractingelement.
 9. An edge-lit waveguide illumination system as recited inclaim 1, further comprising one or more photoresponsive elementsdisposed in an energy receiving relationship with respect to theoptically transmissive plate.
 10. An edge-lit waveguide illuminationsystem as recited in claim 1, further comprising one or more lightconverting elements approximately coextensive with a surface of theoptically transmissive plate and disposed in an energy receivingrelationship with respect to the optically transmissive plate.
 11. Anedge-lit waveguide illumination system as recited in claim 1, whereinthe optically transmissive plate is configured to be bent or flexedwithout breaking.
 12. An edge-lit waveguide illumination system asrecited in claim 1, wherein the optically transmissive plate is retainedin a bent or curved configuration.
 13. An edge-lit waveguideillumination system as recited in claim 1, wherein at least one of theplurality of light emitting diodes is configured to emit monochromaticlight.
 14. An edge-lit waveguide illumination system as recited in claim1, wherein at least one of the light emitting diodes is a side-emittingLED attached to a planar finless heat sink, wherein the planar finlessheat sink is oriented parallel to the optically transmissive plate andcomprises a layer of a metallic material, and wherein a light emittingsurface of the side-emitting LED is oriented perpendicular to aprevalent plane of the planar finless heat sink.
 15. An edge-litwaveguide illumination system as recited in claim 1, wherein at leastone of said light emitting diodes is a side-emitting LED attached to aplanar heat-spreading substrate, wherein the planar heat-spreadingsubstrate is oriented parallel to the optically transmissive plate andperpendicular to a light emitting surface of the side-emitting LED. 16.An edge-lit waveguide illumination system as recited in claim 1, whereina focal length characterizing at least one of the linear cylindricallenses is less than a distance between the lenticular array and theplurality of discrete light extracting surface relief features.
 17. Anedge-lit waveguide illumination system as recited in claim 1, furthercomprising a reflective film laminated to the second edge.
 18. Anedge-lit waveguide illumination system as recited in claim 1, furthercomprising a reflective film laminated to each of the second, third, andfourth edges.
 19. A method of making an edge-lit waveguide illuminationsystem, comprising the steps of: providing a planar monolithic plate ofa rectangular shape from a highly transparent dielectric material at athickness that is at least 40 times less than a major dimension of theplanar monolithic plate; forming a parallel array of linear cylindricallenses in a front surface of the planar monolithic plate such that eachof the linear cylindrical lenses extends between two opposing edges ofthe planar monolithic plate; forming a two dimensional pattern ofdiscrete light extracting surface relief features in an opposing secondsurface of the planar monolithic plate such that the discrete lightextracting surface relief features are separated from each other andfrom all perimeter edges of the planar monolithic plate by smooth andplanar portions of the second surface; positioning a reflective film ona side of the second surface of the planar monolithic plate; positioninga light diffusing layer parallel to the planar monolithic plate; andoptically coupling a plurality of light emitting diodes to a light inputedge of the planar monolithic plate.
 20. A method of making an edge-litwaveguide illumination system as recited in claim 19, wherein the planarmonolithic plate is curved.
 21. A method of making an edge-lit waveguideillumination system as recited in claim 19, further comprising a step ofbending the planar monolithic plate into a curved shape.
 22. A method ofmaking an edge-lit waveguide illumination system as recited in claim 19,further comprising a step of laminating a reflective film to an edge ofthe planar monolithic plate.
 23. A method of making an edge-litwaveguide illumination system as recited in claim 19, further comprisinga step of polishing an edge of the planar monolithic plate.
 24. A methodfor illuminating a display screen comprising: receiving light into alight input edge of a planar optical waveguide having edges disposedbetween a first planar microstructured surface and an opposing secondplanar microstructured surface extending parallel to the first planarmicrostructured surface, wherein the first planar microstructuredsurface defines a parallel array of linear cylindrical lenses extendingalong straight lines between two opposite edges of the planar opticalwaveguide, and wherein the second planar microstructured surfacecomprises a two-dimensional pattern of discrete light extraction surfacerelief features separated from each other and from the edges by smoothand planar portions of the second planar microstructured surface;propagating the light by optical transmission and total internalreflection in an optical material disposed between the first planarmicrostructured surface and the second planar microstructured surfacealong a direction perpendicular to the light input edge, wherein theoptical material has a thickness that is at least 40 times less than alength or width dimension of the second planar microstructured surface;extracting the light from the planar optical waveguide using a pluralityof discrete light extraction surface relief features disrupting totalinternal reflection and causing the light to exit the optical waveguidethrough the first planar microstructured surface and the second planarmicrostructured surface; reflecting at least a portion of the lightexiting through the second planar microstructured surface using areflective surface extending parallel to and approximately coextensivewith the second planar microstructured surface; and distributing thelight through the parallel array of linear cylindrical lenses towardsthe display screen in the form of a divergent beam.